Publications of Ashutosh V. Kotwal    :chronological  combined  by tags listing:

%% Papers Published   
@article{fds376029,
   Author = {ATLAS Collaboration},
   Title = {A detailed map of Higgs boson interactions by the ATLAS
             experiment ten years after the discovery.},
   Journal = {Nature},
   Volume = {607},
   Number = {7917},
   Pages = {52-59},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2022},
   Month = {July},
   url = {http://dx.doi.org/10.1038/s41586-022-04893-w},
   Abstract = {The standard model of particle physics<sup>1-4</sup>
             describes the known fundamental particles and forces that
             make up our Universe, with the exception of gravity. One of
             the central features of the standard model is a field that
             permeates all of space and interacts with fundamental
             particles<sup>5-9</sup>. The quantum excitation of this
             field, known as the Higgs field, manifests itself as the
             Higgs boson, the only fundamental particle with no spin. In
             2012, a particle with properties consistent with the Higgs
             boson of the standard model was observed by the ATLAS and
             CMS experiments at the Large Hadron Collider at
             CERN<sup>10,11</sup>. Since then, more than 30 times as
             many Higgs bosons have been recorded by the ATLAS
             experiment, enabling much more precise measurements and new
             tests of the theory. Here, on the basis of this larger
             dataset, we combine an unprecedented number of production
             and decay processes of the Higgs boson to scrutinize its
             interactions with elementary particles. Interactions with
             gluons, photons, and W and Z bosons-the carriers of the
             strong, electromagnetic and weak forces-are studied in
             detail. Interactions with three third-generation matter
             particles (bottom (b) and top (t) quarks, and tau leptons
             (τ)) are well measured and indications of interactions with
             a second-generation particle (muons, μ) are emerging. These
             tests reveal that the Higgs boson discovered ten years ago
             is remarkably consistent with the predictions of the theory
             and provide stringent constraints on many models of new
             phenomena beyond the standard model.},
   Doi = {10.1038/s41586-022-04893-w},
   Key = {fds376029}
}

@article{fds348468,
   Author = {Kotwal, AV},
   Title = {A fast method for particle tracking and triggering using
             small-radius silicon detectors},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {957},
   Pages = {6 pages},
   Publisher = {Elsevier},
   Year = {2020},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.nima.2020.163427},
   Abstract = {We propose an algorithm, deployable on a highly-parallelized
             graph computing architecture, to perform rapid
             reconstruction of charged-particle trajectories in the high
             energy collisions at the Large Hadron Collider and future
             colliders. We use software emulation to show that the
             algorithm can achieve an efficiency in excess of 99.95% for
             reconstruction with good accuracy. The algorithm can be
             implemented on silicon-based integrated circuits using
             field-programmable gate array technology. Our approach can
             enable a fast trigger for massive charged particles that
             decay invisibly in the tracking volume, as in some
             new-physics scenarios related to particulate dark matter. If
             production of dark matter or other new neutral particles is
             mediated by metastable charged particles and is not
             associated with other triggerable energy deposition in the
             detectors, our method would be useful for triggering on the
             charged mediators using the small-radius silicon
             detectors.},
   Doi = {10.1016/j.nima.2020.163427},
   Key = {fds348468}
}

@article{fds327183,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {A measurement of material in the ATLAS tracker using
             secondary hadronic interactions in 7TeV pp
             collisions},
   Journal = {Journal of Instrumentation},
   Volume = {11},
   Number = {11},
   Pages = {P11020-P11020},
   Publisher = {IOP Publishing},
   Year = {2016},
   Month = {November},
   url = {http://dx.doi.org/10.1088/1748-0221/11/11/P11020},
   Abstract = {Knowledge of the material in the ATLAS inner tracking
             detector is crucial in understanding the reconstruction of
             charged-particle tracks, the performance of algorithms that
             identify jets containing b-hadrons and is also essential to
             reduce background in searches for exotic particles that can
             decay within the inner detector volume. Interactions of
             primary hadrons produced in pp collisions with the material
             in the inner detector are used to map the location and
             amount of this material. The hadronic interactions of
             primary particles may result in secondary vertices, which in
             this analysis are reconstructed by an inclusive
             vertex-finding algorithm. Data were collected using
             minimum-bias triggers by the ATLAS detector operating at the
             LHC during 2010 at centre-of-mass energy √s = 7TeV, and
             correspond to an integrated luminosity of 19nb-1. Kinematic
             properties of these secondary vertices are used to study the
             validity of the modelling of hadronic interactions in
             simulation. Secondary-vertex yields are compared between
             data and simulation over a volume of about 0.7 m3 around the
             interaction point, and agreement is found within overall
             uncertainties.},
   Doi = {10.1088/1748-0221/11/11/P11020},
   Key = {fds327183}
}

@article{fds347490,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini, L and Bianco,
             M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker,
             C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard,
             J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
             A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL},
   Title = {A measurement of the calorimeter response to single hadrons
             and determination of the jet energy scale uncertainty using
             LHC Run-1 pp-collision data with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {1},
   Pages = {26},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4580-0},
   Abstract = {A measurement of the calorimeter response to isolated
             charged hadrons in the ATLAS detector at the LHC is
             presented. This measurement is performed with
             3.2 nb[Formula: see text] of proton-proton collision data
             at [Formula: see text] [Formula: see text] from 2010 and
             0.1 nb[Formula: see text] of data at [Formula: see
             text] [Formula: see text] from 2012. A number of aspects of
             the calorimeter response to isolated hadrons are explored.
             After accounting for energy deposited by neutral particles,
             there is a 5% discrepancy in the modelling, using various
             sets of Geant4 hadronic physics models, of the calorimeter
             response to isolated charged hadrons in the central
             calorimeter region. The description of the response to
             anti-protons at low momenta is found to be improved with
             respect to previous analyses. The electromagnetic and
             hadronic calorimeters are also examined separately, and the
             detector simulation is found to describe the response in the
             hadronic calorimeter well. The jet energy scale uncertainty
             and correlations in scale between jets of different momenta
             and pseudorapidity are derived based on these studies. The
             uncertainty is 2-5% for jets with transverse momenta above
             2 [Formula: see text], where this method provides the jet
             energy scale uncertainty for ATLAS.},
   Doi = {10.1140/epjc/s10052-016-4580-0},
   Key = {fds347490}
}

@article{fds310391,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Bessner, MF and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
             O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
             V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {A measurement of the ratio of the production cross sections
             for [Formula: see text] and [Formula: see text] bosons in
             association with jets with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {12},
   Pages = {3168},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3168-9},
   Abstract = {The ratio of the production cross sections for [Formula: see
             text] and [Formula: see text] bosons in association with
             jets has been measured in proton-proton collisions at
             [Formula: see text] with the ATLAS experiment at the Large
             Hadron Collider. The measurement is based on the entire 2011
             dataset, corresponding to an integrated luminosity of
             [Formula: see text]. Inclusive and differential
             cross-section ratios for massive vector bosons decaying to
             electrons and muons are measured in association with jets
             with transverse momentum [Formula: see text] and jet
             rapidity [Formula: see text]. The measurements are compared
             to next-to-leading-order perturbative QCD calculations and
             to predictions from different Monte Carlo generators
             implementing leading-order matrix elements supplemented by
             parton showers.},
   Doi = {10.1140/epjc/s10052-014-3168-9},
   Key = {fds310391}
}

@article{fds307753,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {A measurement of the ratio of the W and Z cross sections
             with exactly one associated jet in pp collisions at s=7TeV
             with ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {708},
   Number = {3-5},
   Pages = {221-240},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.01.042},
   Abstract = {The ratio of production cross sections of the W and Z bosons
             with exactly one associated jet is presented as a function
             of jet transverse momentum threshold. The measurement has
             been designed to maximise cancellation of experimental and
             theoretical uncertainties, and is reported both within a
             particle-level kinematic range corresponding to the detector
             acceptance and as a total cross-section ratio. Results are
             obtained with the ATLAS detector at the LHC in pp collisions
             at a centre-of-mass energy of 7 TeV using an integrated
             luminosity of 33 pb-1. The results are compared with
             perturbative leading-order, leading-log, and
             next-to-leading-order QCD predictions, and are found to
             agree within experimental and theoretical uncertainties. The
             ratio is measured for events with a single jet with pT>30
             GeV to be 8.73±0.30(stat)±0.40(syst) in the electron
             channel, and 8.49±0.23(stat)±0.33(syst) in the muon
             channel. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.01.042},
   Key = {fds307753}
}

@booklet{Abbott98j,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
             EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis,
             E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram,
             I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del-Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di-Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {A measurement of the W Boson mass at the fermilab pp¯
             Collider},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {14},
   Pages = {3008-3013},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.3008},
   Abstract = {We report a measurement of the W boson mass based on an
             integrated luminosity of 82pb-1 from pp¯ collisions at √s
             = 1.8 TeV recorded in 1994-1995 by the D0 detector at the
             Fermilab Tevatron. We identify W bosons by their decays to
             ev and extract the mass by fitting the transverse mass
             spectrum from 28 323 W boson candidates. A sample of 3563
             dielectron events, mostly due to Z → ee decays, constrains
             models of W boson production and the detector. We measure MW
             = 80.44 ± 0.10(stat) ± 0.07(syst) GeV. By combining this
             measurement with our result form the 1992-1993 data set, we
             obtain MW = 80.43 ± 0.11 GeV. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.80.3008},
   Key = {Abbott98j}
}

@article{fds310358,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyka, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa,
             C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araquea, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik,
             M and Armbruster, AJ and Arnaez, O and Arnal, V},
   Title = {A neural network clustering algorithm for the ATLAS silicon
             pixel detector},
   Journal = {Journal of Instrumentation},
   Volume = {9},
   Number = {9},
   Pages = {P09009-P09009},
   Publisher = {IOP Publishing},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1088/1748-0221/9/09/P09009},
   Abstract = {A novel technique to identify and split clusters created by
             multiple charged particles in the ATLAS pixel detector using
             a set of artificial neural networks is presented. Such
             merged clusters are a common feature of tracks originating
             from highly energetic objects, such as jets. Neural networks
             are trained using Monte Carlo samples produced with a
             detailed detector simulation. This technique replaces the
             former clustering approach based on a connected component
             analysis and charge interpolation. The performance of the
             neural network splitting technique is quantified using data
             from proton-proton collisions at the LHC collected by the
             ATLAS detector in 2011 and from Monte Carlo simulations.
             This technique reduces the number of clusters shared between
             tracks in highly energetic jets by up to a factor of three.
             It also provides more precise position and error estimates
             of the clusters in both the transverse and longitudinal
             impact parameter resolution.},
   Doi = {10.1088/1748-0221/9/09/P09009},
   Key = {fds310358}
}

@article{fds315918,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
             J},
   Title = {A new method to distinguish hadronically decaying boosted
             Z bosons from W bosons using the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {238},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4065-1},
   Abstract = {The distribution of particles inside hadronic jets produced
             in the decay of boosted <i>W</i> and <i>Z</i> bosons can be
             used to discriminate such jets from the continuum
             background. Given that a jet has been identified as likely
             resulting from the hadronic decay of a boosted <i>W</i> or
             <i>Z</i> boson, this paper presents a technique for further
             differentiating <i>Z</i> bosons from <i>W</i> bosons. The
             variables used are jet mass, jet charge, and a
             <i>b</i>-tagging discriminant. A likelihood tagger is
             constructed from these variables and tested in the
             simulation of [Formula: see text] for bosons in the
             transverse momentum range 200 GeV [Formula: see
             text] 400 GeV in [Formula: see text] TeV <i>pp</i>
             collisions with the ATLAS detector at the LHC. For
             <i>Z</i>-boson tagging efficiencies of [Formula: see text],
             50, and [Formula: see text], one can achieve [Formula: see
             text]-boson tagging rejection factors ([Formula: see text])
             of 1.7, 8.3 and 1000, respectively. It is not possible to
             measure these efficiencies in the data due to the lack of a
             pure sample of high [Formula: see text], hadronically
             decaying <i>Z</i> bosons. However, the modelling of the
             tagger inputs for boosted <i>W</i> bosons is studied in data
             using a [Formula: see text]-enriched sample of events in
             20.3 fb[Formula: see text] of data at [Formula: see text]
             TeV. The inputs are well modelled within uncertainties,
             which builds confidence in the expected tagger
             performance.},
   Doi = {10.1140/epjc/s10052-016-4065-1},
   Key = {fds315918}
}

@article{fds313582,
   Author = {ATLAS Collaboration},
   Title = {A particle consistent with the Higgs boson observed with the
             ATLAS detector at the Large Hadron Collider.},
   Journal = {Science (New York, N.Y.)},
   Volume = {338},
   Number = {6114},
   Pages = {1576-1582},
   Publisher = {American Association for the Advancement of Science
             (AAAS)},
   Year = {2012},
   Month = {December},
   ISSN = {0036-8075},
   url = {http://dx.doi.org/10.1126/science.1232005},
   Abstract = {Nearly 50 years ago, theoretical physicists proposed that a
             field permeates the universe and gives energy to the vacuum.
             This field was required to explain why some, but not all,
             fundamental particles have mass. Numerous precision
             measurements during recent decades have provided indirect
             support for the existence of this field, but one crucial
             prediction of this theory has remained unconfirmed despite
             30 years of experimental searches: the existence of a
             massive particle, the standard model Higgs boson. The ATLAS
             experiment at the Large Hadron Collider at CERN has now
             observed the production of a new particle with a mass of 126
             giga-electron volts and decay signatures consistent with
             those expected for the Higgs particle. This result is strong
             support for the standard model of particle physics,
             including the presence of this vacuum field. The existence
             and properties of the newly discovered particle may also
             have consequences beyond the standard model
             itself.},
   Doi = {10.1126/science.1232005},
   Key = {fds313582}
}

@article{fds225678,
   Author = {A.V. Kotwal and T. Aaltonen et al (CDF Collaboration)},
   Title = {A precise measurement of the W-boson mass with the Collider
             Detector at Fermilab},
   Journal = {Phys. Rev. D},
   Volume = {89},
   Number = {072003},
   Year = {2014},
   Month = {Spring},
   Key = {fds225678}
}

@article{fds321115,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {A search for an excited muon decaying to a muon and two jets
             in pp collisions at √ s = 8 TeV with the ATLAS
             detector},
   Journal = {New Journal of Physics},
   Volume = {18},
   Number = {7},
   Pages = {073021-073021},
   Publisher = {IOP Publishing},
   Year = {2016},
   Month = {July},
   url = {http://dx.doi.org/10.1088/1367-2630/18/7/073021},
   Abstract = {Anew search signature for excited leptons is explored.
             Excited muons are sought in the channel pp → μμ∗→
             μμ jet jet, assuming both the production and decay occur
             via a contact interaction. The analysis is based on 20.3
             fb-1 of pp collision data at a centre-of-mass energy of s =
             8 TeV taken with the ATLAS detector at the large hadron
             collider. No evidence of excited muons is found, and limits
             are set at the 95% confidence level on the cross section
             times branching ratio as a function of the excited-muonmass
             μμ∗. For μμ∗between 1.3 and 3.0 TeV, the upper limit
             on φB (μ∗→ μqq) is between 0.6 and 1 fb. Limits on sB
             are converted to lower bounds on the compositeness scale. In
             the limiting case L = μμ∗, excitedmuonswith amass
             below2.8 TeVare excluded.With the samemodel assumptions,
             these limits at larger μ∗masses improve upon previous
             limits fromtraditional searches based on the gauge-mediated
             decay μ∗→ μγ.},
   Doi = {10.1088/1367-2630/18/7/073021},
   Key = {fds321115}
}

@article{fds307687,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
             A and Artoni, G},
   Title = {A search for flavour changing neutral currents in top-quark
             decays in pp collision data collected with the ATLAS
             detector at √s = 7 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {9},
   Pages = {1-36},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2012)139},
   Abstract = {A search for flavour changing neutral current (FCNC)
             processes in top-quark decays by the ATLAS Collaboration is
             presented. Data collected from pp collisions at the LHC at a
             centre-of-mass energy of √s = 7 TeV during 2011,
             corresponding to an integrated luminosity of 2.1 fb-1, were
             used. A search was performed for top-quark pair-production
             events, with one top quark decaying through the t → Zq
             FCNC (q = u, c) channel, and the other through the Standard
             Model dominant mode t → Wb. Only the decays of the Z boson
             to charged leptons and leptonic W-boson decays were
             considered as signal. Consequently, the final-state topology
             is characterised by the presence of three isolated charged
             leptons, at least two jets and missing transverse momentum
             from the undetected neutrino. No evidence for an FCNC signal
             was found. An upper limit on the t → Zq branching ratio of
             BR(t → Zq) < 0.73% is set at the 95% confidence level.
             Copyright CERN.},
   Doi = {10.1007/JHEP09(2012)139},
   Key = {fds307687}
}

@article{fds307624,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, R and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
             Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
             V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia,
             A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
             JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, R and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, R and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Gimenez, VC and Castro,
             NF and Cataldi, G and Catastini, R and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, R and Citron, ZH and Citterio, M and Ciubancan, M and Clark,
             A},
   Title = {A search for high-mass resonances decaying to
             τ+τ- in pp collisions at
             √s=7 TeV with the ATLAS detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {719},
   Number = {4-5},
   Pages = {242-260},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.040},
   Abstract = {© 2012 CERN This Letter presents a search for high-mass
             resonances decaying into τ+τ− final states using
             proton-proton collisions at s=7 TeV produced by the Large
             Hadron Collider. The data were recorded with the ATLAS
             detector and correspond to an integrated luminosity of 4.6
             fb−1. No statistically significant excess above the
             Standard Model expectation is observed; 95% credibility
             upper limits are set on the cross section times branching
             fraction of Z′ resonances decaying into τ+τ− pairs as
             a function of the resonance mass. As a result, Z′ bosons
             of the Sequential Standard Model with masses less than 1.40
             TeV are excluded at 95% credibility.},
   Doi = {10.1016/j.physletb.2013.01.040},
   Key = {fds307624}
}

@article{fds310274,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
             M},
   Title = {A search for high-mass resonances decaying to
             τ+τ in pp collisions at √s =8
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {7},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2015)157},
   Abstract = {Abstract: A search for high-mass resonances decaying into
             τ+τ− final states using proton-proton collisions at
             s=8$$ \sqrt{s}=8 $$ TeV produced by the Large Hadron
             Collider is presented. The data were recorded with the ATLAS
             detector and correspond to an integrated luminosity of
             19.5–20.3 fb−1. No statistically significant excess
             above the Standard Model expectation is observed; 95%
             credibility upper limits are set on the cross section times
             branching fraction of Z′ resonances decaying into τ+τ−
             pairs as a function of the resonance mass. As a result, Z′
             bosons of the Sequential Standard Model with masses less
             than 2.02 TeV are excluded at 95% credibility. The impact of
             the fermionic couplings on the Z′ acceptance is
             investigated and limits are also placed on a Z′ model that
             exhibits enhanced couplings to third-generation
             fermions.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP07(2015)157},
   Key = {fds310274}
}

@article{fds347474,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines,
             JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann,
             TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
             NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
             TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ},
   Title = {A search for pair-produced resonances in four-jet final
             states at s = 13 TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {3},
   Pages = {250},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-5693-4},
   Abstract = {A search for massive coloured resonances which are
             pair-produced and decay into two jets is presented. The
             analysis uses 36.7 fb - 1 of s = 13 TeV <i>pp</i> collision
             data recorded by the ATLAS experiment at the LHC in 2015 and
             2016. No significant deviation from the background
             prediction is observed. Results are interpreted in a SUSY
             simplified model where the lightest supersymmetric particle
             is the top squark, t ~ , which decays promptly into two
             quarks through <i>R</i>-parity-violating couplings. Top
             squarks with masses in the range 100 GeV < m t ~ < 410  
             GeV are excluded at 95% confidence level. If the decay is
             into a <i>b</i>-quark and a light quark, a dedicated
             selection requiring two <i>b</i>-tags is used to exclude
             masses in the ranges 100 GeV < m t ~ < 470   GeV and 480
             GeV < m t ~ < 610   GeV . Additional limits are set on the
             pair-production of massive colour-octet resonances.},
   Doi = {10.1140/epjc/s10052-018-5693-4},
   Key = {fds347474}
}

@article{fds307625,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung,
             C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker,
             S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
             DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
             JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet,
             NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
             S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, E and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran,
             J},
   Title = {A search for prompt lepton-jets in pp collisions at
             √s=7 TeV with the ATLAS detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {719},
   Number = {4-5},
   Pages = {299-317},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.034},
   Abstract = {© 2013 CERN We present a search for a light (mass <2GeV)
             boson predicted by Hidden Valley supersymmetric models that
             decays into a final state consisting of collimated muons or
             electrons, denoted “lepton-jets”. The analysis uses
             5fb−1 of s=7TeV proton–proton collision data recorded by
             the ATLAS detector at the Large Hadron Collider to search
             for the following signatures: single lepton-jets with at
             least four muons; pairs of lepton-jets, each with two or
             more muons; and pairs of lepton-jets with two or more
             electrons. This study finds no statistically significant
             deviation from the Standard Model prediction and places 95%
             confidence-level exclusion limits on the production cross
             section times branching ratio of light bosons for several
             parameter sets of a Hidden Valley model.},
   Doi = {10.1016/j.physletb.2013.01.034},
   Key = {fds307625}
}

@article{fds356783,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {A search for prompt lepton-jets in pp collisions at √s = 8
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {2},
   Pages = {1-51},
   Year = {2016},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP02(2016)062},
   Abstract = {Abstract: A search is presented for a new, light boson with
             a mass of about 1 GeV and decaying promptly to jets of
             collimated electrons and/or muons (lepton-jets). The
             analysis is performed with 20.3 fb−1 of data collected by
             the ATLAS detector at the Large Hadron Collider in
             proton-proton collisions at a centre-of-mass energy of 8
             TeV. Events are required to contain at least two
             lepton-jets. This study finds no statistically significant
             deviation from predictions of the Standard Model and places
             95% confidence-level upper limits on the contribution of new
             phenomena beyond the SM, incuding SUSY-portal and
             Higgs-portal models, on the number of events with
             lepton-jets.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP02(2016)062},
   Key = {fds356783}
}

@article{fds356688,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
             P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {A search for resonances decaying into a Higgs boson and a
             new particle X in the XH → qqbb final state with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {779},
   Pages = {24-45},
   Year = {2018},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.01.042},
   Abstract = {A search for heavy resonances decaying into a Higgs boson
             (H) and a new particle (X) is reported, utilizing 36.1
             fb−1 of proton–proton collision data at s=13TeV
             collected during 2015 and 2016 with the ATLAS detector at
             the CERN Large Hadron Collider. The particle X is assumed to
             decay to a pair of light quarks, and the fully hadronic
             final state XH→qq¯′bb¯ is analysed. The search
             considers the regime of high XH resonance masses, where the
             X and H bosons are both highly Lorentz-boosted and are each
             reconstructed using a single jet with large radius
             parameter. A two-dimensional phase space of XH mass versus X
             mass is scanned for evidence of a signal, over a range of XH
             resonance mass values between 1 TeV and 4 TeV, and for X
             particles with masses from 50 GeV to 1000 GeV. All search
             results are consistent with the expectations for the
             background due to Standard Model processes, and 95% CL upper
             limits are set, as a function of XH and X masses, on the
             production cross-section of the XH→qq¯′bb¯
             resonance.},
   Doi = {10.1016/j.physletb.2018.01.042},
   Key = {fds356688}
}

@article{fds308097,
   Author = {Abulencia, and A, and others},
   Title = {A search for scalar bottom quarks from gluino decays in
             $\bar{p}p$ collisions at $\sqrt{s} =$ 1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {17},
   Pages = {171802},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.171802},
   Abstract = {We searched for scalar bottom quarks in 156 pb-1 of p anti-p
             collisions at s**(1/2) = 1.96 TeV recorded by the CDF II
             experiment at the Tevatron. Scalar bottom quarks can be
             produced from gluino decays in R-parity conserving models of
             supersymmetry when the mass of the gluino exceeds that of
             the scalar bottom quark. Then, a scalar bottom quark. Then,
             a scalar bottom quark can decay into a bottom quark and a
             neutralino. To search for this scenario, we investigated
             events with large missing transverse energy and at least
             three jets, two or more of which were identified as
             containing a secondary vertex from the hadronization of b
             quarks. We found four candidate events, where 2.6 +/- 0.7
             are expected from standard model processes, and placed 95\%
             confidence level lower limits on gluino and scalar bottom
             quark masses of up to 280 and 240 GeV/c2,
             respectively.},
   Doi = {10.1103/physrevlett.96.171802},
   Key = {fds308097}
}

@article{fds308110,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
             J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
             J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH},
   Title = {A search for t → τ ν q in t over(t, ̄)
             production},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {639},
   Number = {3-4},
   Pages = {172-178},
   Publisher = {Elsevier BV},
   Year = {2006},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2006.06.030},
   Abstract = {We present a search for t over(t, ̄) events with a tau
             lepton in the final state. The data sample corresponds to an
             integrated luminosity of 194 pb-1 collected with the CDF II
             detector from p over(p, ̄) collisions at a center of mass
             energy of 1.96 TeV. We observe two events with an expected
             signal of 1.0 ± 0.2 events and a background of 1.3 ± 0.3
             events. We determine a 95% confidence level upper limit on
             rτ, the ratio of the measured rate of t → τ ν q to the
             expectation, of 5.2. © 2006 Elsevier B.V. All rights
             reserved.},
   Doi = {10.1016/j.physletb.2006.06.030},
   Key = {fds308110}
}

@article{fds366276,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
             JF},
   Title = {A search for the decays of stopped long-lived particles at
             √s = 13 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {7},
   Year = {2021},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2021)173},
   Abstract = {A search for long-lived particles, which have come to rest
             within the ATLAS detector, is presented. The subsequent
             decays of these particles can produce high-momentum jets,
             resulting in large out-of-time energy deposits in the ATLAS
             calorimeters. These de- cays are detected using data
             collected during periods in the LHC bunch structure when
             collisions are absent. The analysed dataset is composed of
             events from proton-proton collisions produced by the Large
             Hadron Collider at a centre-of-mass energy of s = 13 TeV and
             recorded by the ATLAS experiment during 2017 and 2018. The
             dataset used for this search corresponds to a total live
             time of 579 hours. The results of this search are used to
             derive lower limits on the mass of gluino R-hadrons,
             assuming a branching fraction B(g~→qq¯χ10) = 100%, with
             masses of up to 1.4 TeV excluded for gluino lifetimes of
             10−5 to 103 s. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP07(2021)173},
   Key = {fds366276}
}

@article{fds307941,
   Author = {al, AVKWTAE and Collaboration, CDF},
   Title = {A Search for the Higgs Boson Produced in Association with
             Z-> l+ l- Using the Matrix Element Method at CDF
             II},
   Journal = {Physical Review D},
   Volume = {80},
   Number = {071101 (R)},
   Pages = {8},
   Year = {2009},
   Month = {Fall},
   Key = {fds307941}
}

@article{fds307905,
   Author = {Aaltonen, and T, and others},
   Title = {A Search for the Higgs Boson Using Neural Networks in Events
             with Missing Energy and $b$-quark Jets in $p\bar p$
             Collisions at $\sqrt{s}=1.96$ TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {14},
   Pages = {141801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.141801},
   Abstract = {http://arxiv.org/abs/0911.3935},
   Doi = {10.1103/PhysRevLett.104.141801},
   Key = {fds307905}
}

@article{fds352891,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {A search for the Zγ decay mode of the Higgs boson in pp
             collisions at s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {809},
   Year = {2020},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2020.135754},
   Abstract = {A search for the Zγ decay of the Higgs boson, with Z boson
             decays into pairs of electrons or muons is presented. The
             analysis uses proton–proton collision data at s = 13 TeV
             corresponding to an integrated luminosity of 139 fb−1
             recorded by the ATLAS detector at the Large Hadron Collider.
             The observed data are consistent with the expected
             background with a p-value of 1.3%. An upper limit at 95%
             confidence level on the production cross-section times the
             branching ratio for pp→H→Zγ is set at 3.6 times the
             Standard Model prediction while 2.6 times is expected in the
             presence of the Standard Model Higgs boson. The best-fit
             value for the signal yield normalised to the Standard Model
             prediction is 2.0−0.9+1.0 where the statistical component
             of the uncertainty is dominant.},
   Doi = {10.1016/j.physletb.2020.135754},
   Key = {fds352891}
}

@article{fds321123,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {A search for top squarks with R-parity-violating decays to
             all-hadronic final states with the ATLAS detector in √s =
             8 TeV proton-proton collisions},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {6},
   Pages = {1-49},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2016)067},
   Abstract = {A search for the pair production of top squarks, each with
             R-parity-violating decays into two Standard Model quarks, is
             performed using 17.4 fb−1 of √s = 8 TeV proton-proton
             collision data recorded by the ATLAS experiment at the LHC.
             Each top squark is assumed to decay to a b- and an s-quark,
             leading to four quarks in the final state. Background
             discrimination is achieved with the use of b-tagging and
             selections on the mass and substructure of large-radius
             jets, providing sensitivity to top squark masses as low as
             100 GeV. No evidence of an excess beyond the Standard Model
             background prediction is observed and top squarks decaying
             to b¯ s¯ are excluded for top squark masses in the range
             100 ≤ mt≤ 315 GeV at 95% confidence level.},
   Doi = {10.1007/JHEP06(2016)067},
   Key = {fds321123}
}

@article{fds315360,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
             G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {A search for tt resonances using lepton-plus-jets events in
             proton-proton collisions at √s=8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2015)148},
   Abstract = {Abstract: A search for new particles that decay into top
             quark pairs is reported. The search is performed with the
             ATLAS experiment at the LHC using an integrated luminosity
             of 20.3 fb−1 of proton-proton collision data collected at
             a centre-of-mass energy of √s=8 TeV. The lepton-plus-jets
             final state is used, where the top pair decays to
             W+bW−b¯, with one W boson decaying leptonically and the
             other hadronically. The invariant mass spectrum of top quark
             pairs is examined for local excesses or deficits that are
             inconsistent with the Standard Model predictions. No
             evidence for a top quark pair resonance is found, and 95%
             confidence-level limits on the production rate are
             determined for massive states in benchmark models. The upper
             limits on the cross-section times branching ratio of a
             narrow Z′ boson decaying to top pairs range from 4.2 pb to
             0.03 pb for resonance masses from 0.4 TeV to 3.0 TeV. A
             narrow leptophobic topcolour Z′ boson with mass below 1.8
             TeV is excluded. Upper limits are set on the cross-section
             times branching ratio for a broad colour-octet resonance
             with Γ/m = 15% decaying to tt¯. These range from 4.8 pb to
             0.03 pb for masses from 0.4 TeV to 3.0 TeV. A Kaluza-Klein
             excitation of the gluon in a Randall-Sundrum model is
             excluded for masses below 2.2 TeV.},
   Doi = {10.1007/JHEP08(2015)148},
   Key = {fds315360}
}

@article{fds307784,
   Author = {ATLAS Collaboration},
   Title = {A search for ttbar resonances with the ATLAS detector in
             2.05 fb^-1 of proton-proton collisions at sqrt(s) = 7
             TeV},
   Journal = {The European Physical Journal C},
   Volume = {72},
   Number = {7},
   Pages = {2083},
   Year = {2012},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2083-1},
   Abstract = {A search for top quark pair resonances in final states
             containing at least one electron or muon has been performed
             with the ATLAS experiment at the CERN Large Hadron Collider.
             The search uses a data sample corresponding to an integrated
             luminosity of 2.05 fb<sup>-1</sup>, which was recorded in
             2011 at a proton-proton centre-of-mass energy of 7 TeV. No
             evidence for a resonance is found and limits are set on the
             production cross-section times branching ratio to [Formula:
             see text] for narrow and wide resonances. For narrow
             <i>Z</i>' bosons, the observed 95 % Bayesian credibility
             level limits range from 9.3 pb to 0.95 pb for masses in
             the range of <i>m</i><sub><i>Z</i>'</sub>=500 GeV to
             <i>m</i><sub><i>Z</i>'</sub>=1300 GeV. The corresponding
             excluded mass region for a leptophobic topcolour <i>Z</i>'
             boson (Kaluza-Klein gluon excitation in the Randall-Sundrum
             model) is <i>m</i><sub><i>Z</i>'</sub><880 GeV ([Formula:
             see text]).},
   Doi = {10.1140/epjc/s10052-012-2083-1},
   Key = {fds307784}
}

@article{fds212566,
   Author = {A.V. Kotwal and ATLAS Collaboration},
   Title = {A search for ttbar resonances with the ATLAS detector in
             2.05/fb of proton-proton collisions at √s=7
             TeV},
   Journal = {Eur. Phys. J. C},
   Volume = {72},
   Pages = {2083},
   Year = {2012},
   Month = {July},
   Key = {fds212566}
}

@article{fds307721,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {A search for tt̄ resonances in lepton+jets events with
             highly boosted top quarks collected in pp collisions at √s
             = 7TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP09(2012)041},
   Abstract = {A search for resonant production of high-mass top-quark
             pairs is performed on 2.05 fb-1 of proton-proton collisions
             at √s = 7 TeV collected in 2011 with the ATLAS experiment
             at the Large Hadron Collider. This analysis of the
             lepton+jets final state is specifically designed for the
             particular topology that arises from the decay of highly
             boosted top quarks. The observed tt̄ invariant mass
             spectrum is found to be compatible with the Standard Model
             prediction and 95% credibility level upper limits are
             derived on the tt̄ production rate through new massive
             states. An upper limit of 0.7 pb is set on the production
             cross section times branching fraction of a narrow 1 TeV
             resonance. A Kaluza-Klein gluon with a mass smaller than 1.5
             TeV is excluded.},
   Doi = {10.1007/JHEP09(2012)041},
   Key = {fds307721}
}

@article{fds356626,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {A strategy for a general search for new phenomena using
             data-derived signal regions and its application within the
             ATLAS experiment},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {2},
   Year = {2019},
   Month = {February},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-6540-y},
   Abstract = {This paper describes a strategy for a general search used by
             the ATLAS Collaboration to find potential indications of new
             physics. Events are classified according to their final
             state into many event classes. For each event class an
             automated search algorithm tests whether the data are
             compatible with the Monte Carlo simulated expectation in
             several distributions sensitive to the effects of new
             physics. The significance of a deviation is quantified using
             pseudo-experiments. A data selection with a significant
             deviation defines a signal region for a dedicated follow-up
             analysis with an improved background expectation. The
             analysis of the data-derived signal regions on a new dataset
             allows a statistical interpretation without the large
             look-elsewhere effect. The sensitivity of the approach is
             discussed using Standard Model processes and benchmark
             signals of new physics. As an example, results are shown for
             3.2 fb- 1 of proton–proton collision data at a
             centre-of-mass energy of 13 TeV collected with the ATLAS
             detector at the LHC in 2015, in which more than 700 event
             classes and more than 10 5 regions have been analysed. No
             significant deviations are found and consequently no
             data-derived signal regions for a follow-up analysis have
             been defined.},
   Doi = {10.1140/epjc/s10052-019-6540-y},
   Key = {fds356626}
}

@article{fds346178,
   Author = {Kotwal, J and Singh, V and Kotwal, A and Dutta, V and Nair,
             V},
   Title = {A study of haematological and bone marrow changes in
             symptomatic patients with human immune deficiency virus
             infection with special mention of functional iron
             deficiency, anaemia of critically ill and haemophagocytic
             lymphohistiocytosis.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {69},
   Number = {4},
   Pages = {319-325},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.mjafi.2012.11.002},
   Abstract = {<h4>Background</h4>Haematological abnormalities are among
             the most common complications of HIV. These involve all
             lineages of blood cells. Bone marrow studies form integral
             part of complete workup of the HIV positive patients
             specially when they present as case of pyrexia of unknown
             origin (PUO), refractory anaemia and pancytopenia.<h4>Method</h4>55
             HIV infected symptomatic patient requiring bone marrow
             examination were included in the study. Relevant clinical
             history, baseline haematological investigations including
             full blood count, CD4 cell counts using flow cytometry were
             recorded.<h4>Results</h4>Median ANC values in males were
             found to be significantly lower than females (p = 0.046).
             CD4 cell count statistically significantly correlated with
             age, TLC, ANC & platelet count. Anaemia was present in 45
             patients and out of which 66.66% patients had normocytic
             normochromic anaemia. Iron deficiency anaemia was present in
             (37.77%) patients and anaemia of chronic disease in (62.22%)
             patients. 2 patients had anaemia of the critically ill. Two
             patients had non-Hodgkin's lymphoma (NHL) and showed
             lymphoma deposit in the bone marrow. Gelatinous degeneration
             was seen in 3 patients. Ill formed epithelioid cell
             granulomas were seen in 7 cases, and 2 cases were positive
             for acid fast bacilli (AFB). Haemophagocytosis was seen in 8
             cases; two cases later diagnosed as a case of infection
             induced HLH. Leishmania donovani (LD) bodies seen in 2
             cases.<h4>Conclusions</h4>Bone marrow study is an important
             investigation in HIV infected symptomatic patients with
             peripheral haematological abnormalities.},
   Doi = {10.1016/j.mjafi.2012.11.002},
   Key = {fds346178}
}

@article{fds346170,
   Author = {Kotwal, A and Singh, H and Verma, AK and Gupta, RM and Jain, S and Sinha,
             S and Joshi, RK and Teli, P and Khunga, V and Bhatnagar, A and Ranjan,
             R},
   Title = {A study of Hepatitis A and E virus seropositivity profile
             amongst young healthy adults in India.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {70},
   Number = {3},
   Pages = {225-229},
   Year = {2014},
   Month = {July},
   url = {http://dx.doi.org/10.1016/j.mjafi.2014.06.016},
   Abstract = {<h4>Background</h4>Various Serosurveys and studies provide
             ample evidence of differing perspectives regarding
             epidemiology of HAV and HEV in India. This study was
             conducted to assess the seroprevalence of HAV and HEV and
             its associated factors with an aim to provide inputs to
             planners regarding requirement of HAV vaccine.<h4>Methods</h4>A
             multi-centric cross sectional survey amongst 4175 healthy
             trainees (young adults) was carried out in training centres,
             selected by multistage random sampling, giving equal
             representation to all regions of India. Sample size was
             calculated by taking prevalence of HAV seropositivity
             amongst adults as 60% and alpha 0.05.<h4>Results</h4>Seroprevalence
             for HAV and HEV was 92.68% (95% CI 91.82, 93.47) and 17.05%
             (15.90, 18.26), respectively. Logistic regression showed
             that hand washing without soap, regular close contact with
             domestic animals, consumption of unpasteurized milk and
             regular consumption of food outside home were risk factors
             for HAV (p < 0.05). For HEV, irregular hand washing,
             consumption of unpasteurized milk and irregular consumption
             of freshly prepared food were risk factors
             (p < 0.05).<h4>Conclusion</h4>High level of immunity
             against HAV among the healthy young adults clearly
             demonstrates that vaccination against HAV is not required at
             present in our country. The large proportion being
             susceptible to HEV points towards the requirement of
             preventive strategies in the form of safe drinking water
             supply, hygiene, sanitation, increasing awareness and
             behaviour change with respect to personal hygiene especially
             hand and food hygiene.},
   Doi = {10.1016/j.mjafi.2014.06.016},
   Key = {fds346170}
}

@article{fds307928,
   Author = {Aaltonen, and T, and others},
   Title = {A study of the associated production of photons and
             $b$-quark jets in $p \bar{p}$ collisions at $\sqrt{s} =
             1.96$ TeV},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {5},
   Pages = {052006},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.052006},
   Abstract = {http://arxiv.org/abs/0912.3453},
   Doi = {10.1103/PhysRevD.81.052006},
   Key = {fds307928}
}

@article{fds307762,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {A study of the material in the ATLAS inner detector using
             secondary hadronic interactions},
   Journal = {Journal of Instrumentation},
   Volume = {7},
   Number = {1},
   Pages = {P01013-P01013},
   Publisher = {IOP Publishing},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1748-0221/7/01/P01013},
   Abstract = {The ATLAS inner detector is used to reconstruct secondary
             vertices due to hadronic interactions of primary collision
             products, so probing the location and amount of material in
             the inner region of ATLAS. Data collected in 7 TeV pp
             collisions at the LHC, with a minimum bias trigger, are used
             for comparisons with simulated events. The reconstructed
             secondary vertices have spatial resolutions ranging from ∼
             200μm to 1 mm. The overall material description in the
             simulation is validated to within an experimental
             uncertainty of about 7%. This will lead to a better
             understanding of the reconstruction of various objects such
             as tracks, leptons, jets, and missing transverse momentum.
             © 2012 CERN.},
   Doi = {10.1088/1748-0221/7/01/P01013},
   Key = {fds307762}
}

@article{fds346189,
   Author = {Seth, T and Kotwal, A and Thakur, RK and Ganguly,
             KK},
   Title = {A study on community perceptions of common cancers,
             determinants of community behaviour and program
             implementation in New Delhi, India.},
   Journal = {Asian Pacific journal of cancer prevention :
             APJCP},
   Volume = {13},
   Number = {6},
   Pages = {2781-2789},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.7314/apjcp.2012.13.6.2781},
   Abstract = {Assessment of perceptions of the community, the determinants
             and development of their behavior regarding common
             malignancies, helps in establishing evidence-based
             activities for prevention and early diagnosis of cancer.
             However information on this important aspect is lacking in
             our country. Qualitative methods were here used to obtain
             information through in depth interviews and Focus Group
             Discussions (FGDs) with all categories of identified
             stakeholders. Most were unaware of the activities of the
             cancer control program. Even the providers were not fully
             conversant. All respondents mentioned lack of diagnostic and
             treatment facilities in government, primary and secondary
             level facilities. Perceptions of different categories of
             stakeholders regarding why many community members did not
             attend screening camps and other services reflect the
             determinants of community behavior, acting independently as
             well as in combination. The cancer control program was
             thought to be restricted only to some private facilities and
             overcrowded government tertiary care facilities where the
             visits were time consuming. Almost all the facilities were
             considered curative oriented. Issues of supervision,
             monitoring and feedback were inadequately addressed by
             providers who were inadequately trained in many program
             activities. The program lacked effective planning,
             coordination and appropriate implementation at the grass
             roots level in Delhi. Social mobilization was grossly
             inadequate, as most of the community members were unaware of
             the existence of the program. Misconceptions about the risk
             factors, signs and symptoms, diagnosis, and treatment were
             common amongst community members as well as many of the
             providers. Thus the national cancer control program in our
             country needs further community participation and social
             mobilization. Accessibility, availability, acceptability and
             affordability of various preventive, curative and
             rehabilitative activities, as well as intersectoral
             coordination, training, supervision and monitoring of
             program activities, all need to be addressed to ensure the
             success of this important public health program.},
   Doi = {10.7314/apjcp.2012.13.6.2781},
   Key = {fds346189}
}

@article{fds347534,
   Author = {Goel, N and Khandelwal, V and Pandya, K and Kotwal,
             A},
   Title = {Alcohol and Tobacco Use Among Undergraduate and Postgraduate
             Medical Students in India: A Multicentric Cross-sectional
             Study.},
   Journal = {Central Asian journal of global health},
   Volume = {4},
   Number = {1},
   Pages = {187},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.5195/cajgh.2015.187},
   Abstract = {<h4>Background</h4>Substance use among medical fraternity is
             a well-known phenomenon among both undergraduate (UG) and
             postgraduate (PG) medical students. Yet, there have been
             very few multi-centric studies to estimate the actual burden
             of this problem in this important population group in India.
             This study was conducted to estimate the prevalence of
             alcohol and tobacco use, assess the knowledge and attitudes
             towards this issue, and identify factors associated with
             substance use among UG and PG medical students in
             India.<h4>Methods</h4>A pre-tested, self-report, anonymous
             questionnaire was administered to medical undergraduates and
             post graduate medical residents of eight medical colleges
             across India. This study used a convenience sample of
             medical colleges with random selection of study participants
             within each college for each group, UG and
             PG.<h4>Results</h4>Prevalence of alcohol and tobacco use
             among UG students was 16.6%, 95% CI [14.5, 18.9] and 8.0%,
             95% CI [6.4, 9.6], respectively, whereas prevalence was
             31.5%, 95% CI [26.3, 37.0] and 14.5%, 95% CI [10.7, 18.9],
             respectively for PGs. For both substances, males had a
             higher prevalence of use compared to females in both groups
             (<i>p</i> < 0.001). Positive family history of substance use
             (<i>p</i> < 0.001 for both groups) and early age of
             initiation (<i>p</i> = 0.011 for tobacco; <i>p</i> > 0.05
             for alcohol) were associated with a greater difficulty to
             quit the habit. Over 90% of study participants felt that
             substance use adversely affected their skills and reported
             not using substances prior to managing their
             patients.<h4>Conclusions</h4>Since substance use is a
             relatively common phenomenon among UG and PG medical
             students in India, future prospective studies and
             interventions are required to better understand the pattern
             of substance use and reduce its prevalence.},
   Doi = {10.5195/cajgh.2015.187},
   Key = {fds347534}
}

@article{fds354613,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
             KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
   Title = {Alignment of the ATLAS Inner Detector in Run
             2},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {12},
   Year = {2020},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-08700-6},
   Abstract = {The performance of the ATLAS Inner Detector alignment has
             been studied using pp collision data at s=13TeV collected by
             the ATLAS experiment during Run 2 (2015–2018) of the Large
             Hadron Collider (LHC). The goal of the detector alignment is
             to determine the detector geometry as accurately as possible
             and correct for time-dependent movements. The Inner Detector
             alignment is based on the minimization of track-hit
             residuals in a sequence of hierarchical levels, from global
             mechanical assembly structures to local sensors. Subsequent
             levels have increasing numbers of degrees of freedom; in
             total there are almost 750,000. The alignment determines
             detector geometry on both short and long timescales, where
             short timescales describe movements within an LHC fill. The
             performance and possible track parameter biases originating
             from systematic detector deformations are evaluated.
             Momentum biases are studied using resonances decaying to
             muons or to electrons. The residual sagitta bias and
             momentum scale bias after alignment are reduced to less than
             ∼0.1TeV-1 and 0.9 × 10 - 3, respectively. Impact
             parameter biases are also evaluated using tracks within
             jets.},
   Doi = {10.1140/epjc/s10052-020-08700-6},
   Key = {fds354613}
}

@article{fds347526,
   Author = {Biswas, D and Kotwal, A and Kakati, B and Ahmad, S},
   Title = {Amphotericin B Resistant Apophysomyces elegans Causing
             Rhino-oculo-Cerebral Mucormycosis in an Immunocompetent
             Host.},
   Journal = {Journal of clinical and diagnostic research :
             JCDR},
   Volume = {9},
   Number = {8},
   Pages = {DD01-DD02},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.7860/jcdr/2015/13929.6272},
   Abstract = {Mucormycosis, an angioinvasive infection is caused by the
             ubiquitous filamentous fungi of the order Mucorales and
             class Mucormycetes. Reports of this disease are on the rise
             over the past few decades. Rhino-oculo-Cerebral presentation
             associated with uncontrolled diabetes is the predominant
             characteristic of this entity. We report here a case of
             rhinooculocerebral mucormycosis (ROCM) due to Apophysomyces
             elegans (A. elegans) in a 45-year-old diabetic lady with
             background illness of hypothyroidism and
             polyradiculoneuropathy. Though this condition is usually
             managed with surgical debridement of the affected tissue and
             medical therapy with Amphotericin B, the isolate recovered
             in our case was found to be resistant to Amphotericin
             B.},
   Doi = {10.7860/jcdr/2015/13929.6272},
   Key = {fds347526}
}

@article{fds346191,
   Author = {Kotwal, A and Biswas, D and Sharma, JP and Gupta, A and Jindal,
             P},
   Title = {An observational study on the epidemiological and
             mycological profile of Candidemia in ICU
             patients.},
   Journal = {Medical science monitor : international medical journal of
             experimental and clinical research},
   Volume = {17},
   Number = {11},
   Pages = {CR663-CR668},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.12659/msm.882053},
   Abstract = {<h4>Background</h4>This study aimed to analyze the
             epidemiological and mycological profile of candidemia in
             intensive care unit (ICU) patients attending a tertiary care
             teaching hospital in the Himalayan region of northern
             India.<h4>Material/methods</h4>A 15-bed medico-surgical ICU
             and a 5-bed pediatric ICU. Ninety-one consecutively admitted
             ICU patients were screened for the presence of candidemia by
             performing blood cultures at periodic intervals.<h4>Results</h4>The
             recovered Candida isolates were speciated and subjected to
             antifungal susceptibility testing using standard procedures.
             Forty-one of the recruited patients (45%) were found to be
             candidemic, with the majority of patients being in the
             extremes of age (13 neonates and 15 >65 years of age). Four
             risk factors were found to be significantly associated with
             the occurrence of candidemia in our patients - a period of
             hospitalization exceeding 7 days (p=0.0008), previous use of
             antibiotics (p=0.001), presence of chronic renal failure
             (p=0.003), and ongoing cancer chemotherapy (p= 0.041).
             Ninety-six Candida isolates were recovered from the 41
             culture-positive patients, with Candida albicans being the
             commonest isolate recovered (n=75, 78.1%), followed by
             Candida tropicalis (n=15, 16%), and Candida glabrata (n=6,
             6.5%). Fluconazole resistance was observed among 26% of all
             Candida isolates and 17.3% of C. albicans
             isolates.<h4>Conclusions</h4>Contrary to the majority of
             recent reports, species shift towards non-albicans
             candidemia has not been observed in our center, though the
             prevalence of azole resistance is alarmingly high even among
             the C. albicans isolates.},
   Doi = {10.12659/msm.882053},
   Key = {fds346191}
}

@article{fds347528,
   Author = {Sahai, K and Kotwal, A},
   Title = {Anaemia prevention in the community: students as change
             agents.},
   Journal = {Medical education},
   Volume = {49},
   Number = {5},
   Pages = {518-519},
   Year = {2015},
   Month = {May},
   url = {http://dx.doi.org/10.1111/medu.12683},
   Doi = {10.1111/medu.12683},
   Key = {fds347528}
}

@article{fds308060,
   Author = {Abulencia, and A, and others},
   Title = {Analysis of the quantum numbers J(PC) of the
             X(3872)},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {13},
   Pages = {132002},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.132002},
   Abstract = {We present an analysis of angular distributions and
             correlations of the X(3872) particle in the exclusive decay
             mode X(3872)-->J/psipi+pi- with J/psi-->µ+µ-. We use 780
             pb-1 of data from p[overline p] collisions at sqrt(s)=1.96
             TeV collected with the CDF II detector at the Fermilab
             Tevatron. We derive constraints on spin, parity, and charge
             conjugation parity of the X(3872) particle by comparing
             measured angular distributions of the decay products with
             predictions for different JPC hypotheses. The assignments
             JPC=1++ and 2-+ are the only ones consistent with the
             data.},
   Doi = {10.1103/physrevlett.98.132002},
   Key = {fds308060}
}

@article{fds356714,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Analysis of the Wtb vertex from the measurement of
             triple-differential angular decay rates of single top quarks
             produced in the t-channel at √s=8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {12},
   Year = {2017},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2017)017},
   Abstract = {The electroweak production and subsequent decay of single
             top quarks in the t-channel is determined by the properties
             of the Wtb vertex, which can be described by the complex
             parameters of an effective Lagrangian. An analysis of a
             triple-differential decay rate in t-channel production is
             used to simultaneously determine five generalised helicity
             fractions and phases, as well as the polarisation of the
             produced top quark. The complex parameters are then
             constrained. This analysis is based on 20.2 fb−1 of
             proton-proton collision data at a centre-of-mass energy of 8
             TeV collected with the ATLAS detector at the LHC. The
             fraction of decays containing transversely polarised W
             bosons is measured to be f1 = 0.30 ± 0.05. The phase
             between amplitudes for transversely and longitudinally
             polarised W bosons recoiling against left-handed b-quarks is
             measured to be δ− = 0.002π+ 0.017π+ 0.016π, giving no
             indication of CP violation. The fractions of longitudinal or
             transverse W bosons accompanied by right-handed b-quarks are
             also constrained. Based on these measurements, limits are
             placed at 95% CL on the ratio of the complex coupling
             parameters Re [gR/VL ∈ [−0.12, 0.17] and Im [gR/VL ∈
             [−0.07, 0.06]. Constraints are also placed on the ratios
             |VR/VL| and |gL/VL|. In addition, the polarisation of single
             top quarks in the t-channel is constrained to be P > 0.72
             (95% CL). None of the above measurements make assumptions
             about the value of any of the other parameters or couplings
             and all of them are in agreement with the Standard
             Model.[Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP12(2017)017},
   Key = {fds356714}
}

@article{fds356655,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson,
             TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold,
             H},
   Title = {Angular analysis of Bd0 → K
              μ + μ  decays in
             pp collisions at √s=8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {10},
   Year = {2018},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2018)047},
   Abstract = {An angular analysis of the decay Bd0 → K∗μ+μ− is
             presented, based on proton-proton collision data recorded by
             the ATLAS experiment at the LHC. The study is using 20.3
             fb−1 of integrated luminosity collected during 2012 at
             centre-of-mass energy of s=8 TeV. Measurements of the K*
             longitudinal polarisation fraction and a set of angular
             parameters obtained for this decay are presented. The
             results are compatible with the Standard Model
             predictions.[Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP10(2018)047},
   Key = {fds356655}
}

@article{fds373908,
   Author = {Amerl, M and Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin,
             T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi,
             G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori,
             G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang,
             R and Zhang, J and Berlendis, S and Cheu, E and Cui, Z and Ghosh, A and Johns,
             KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand,
             HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK},
   Title = {Anomaly detection search for new resonances decaying into a
             Higgs boson and a generic new particle X in hadronic final
             states using Formula Presented pp collisions with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {108},
   Number = {5},
   Year = {2023},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.108.052009},
   Abstract = {A search is presented for a heavy resonance Formula
             Presented decaying into a Standard Model Higgs boson Formula
             Presented and a new particle Formula Presented in a fully
             hadronic final state. The full Large Hadron Collider run 2
             dataset of proton-proton collisions at Formula Presented
             collected by the ATLAS detector from 2015 to 2018 is used
             and corresponds to an integrated luminosity of Formula
             Presented. The search targets the high Formula
             Presented-mass region, where the Formula Presented and
             Formula Presented have a significant Lorentz boost in the
             laboratory frame. A novel application of anomaly detection
             is used to define a general signal region, where events are
             selected solely because of their incompatibility with a
             learned background-only model. It is constructed using a
             jet-level tagger for signal-model-independent selection of
             the boosted Formula Presented particle, representing the
             first application of fully unsupervised machine learning to
             an ATLAS analysis. Two additional signal regions are
             implemented to target a benchmark Formula Presented decay
             into two quarks, covering topologies where the Formula
             Presented is reconstructed as either a single large-radius
             jet or two small-radius jets. The analysis selects Higgs
             boson decays into Formula Presented, and a dedicated
             neural-network-based tagger provides sensitivity to the
             boosted heavy-flavor topology. No significant excess of data
             over the expected background is observed, and the results
             are presented as upper limits on the production cross
             section Formula Presented) for signals with Formula
             Presented between 1.5 and 6 TeV and Formula Presented
             between 65 and 3000 GeV.},
   Doi = {10.1103/PhysRevD.108.052009},
   Key = {fds373908}
}

@article{fds347535,
   Author = {Bangalore, S and Toklu, B and Kotwal, A and Volodarskiy, A and Sharma,
             S and Kirtane, AJ and Feit, F},
   Title = {Anticoagulant therapy during primary percutaneous coronary
             intervention for acute myocardial infarction: a
             meta-analysis of randomized trials in the era of stents and
             P2Y12 inhibitors.},
   Journal = {BMJ (Clinical research ed.)},
   Volume = {349},
   Pages = {g6419},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1136/bmj.g6419},
   Abstract = {<h4>Objectives</h4>To investigate the relative benefits of
             unfractionated heparin, low molecular weight heparin(LMWH),
             fondaparinux, and bivalirudin as treatment options for
             patients with ST segment elevation myocardial infarction
             undergoing percutaneous coronary intervention
             (PCI).<h4>Design</h4>Mixed treatment comparison and direct
             comparison meta-analysis of randomized trials in the era of
             stents and P2Y12 inhibitors.<h4>Data sources and study
             selection</h4>A search of Medline, Embase, Cochrane Central
             Register of Controlled Trials (CENTRAL) for randomized
             trials comparing unfractionated heparin plus glycoprotein
             IIb/IIIa inhibitor(GpIIb/IIIa inhibitor), unfractionated
             heparin, bivalirudin, fondaparinux, or LMWH plus GpIIb/IIIa
             inhibitor for patients undergoing primary
             PCI.<h4>Outcomes</h4>The primary efficacy outcome was short
             term (in hospital or within 30 days) major adverse
             cardiovascular event; the primary safety outcome was short
             term major bleeding.<h4>Results</h4>We identified 22
             randomized trials that enrolled 22,434 patients. In the
             mixed treatment comparison models, when compared with
             unfractionated heparin plus GpIIb/IIIa inhibitor,
             unfractionated heparin was associated with a higher risk of
             major adverse cardiovascular events (relative risk 1.49 (95%
             confidence interval 1.21 to 1.84), as were bivalirudin
             (relative risk 1.34 (1.01 to 1.78)) and fondaparinux (1.78
             (1.01 to 3.14)). LMWH plus GpIIb/IIIa inhibitor showed
             highest treatment efficacy, followed (in order) by
             unfractionated heparin plus GpIIb/IIIa inhibitor,
             bivalirudin, unfractionated heparin, and fondaparinux.
             Bivalirudin was associated with lower major bleeding risk
             compared with unfractionated heparin plus GpIIb/IIIa
             inhibitor (relative risk 0.47 (0.30 to 0.74)) or
             unfractionated heparin (0.58 (0.37 to 0.90)). Bivalirudin,
             followed by unfractionated heparin, LMWH plus GpIIb/IIIa
             inhibitor, unfractionated heparin plus GpIIb/IIIa inhibitor,
             and fondaparinux were the hierarchy for treatment safety.
             Results were similar in direct comparison meta-analyses:
             bivalirudin was associated with a 39%, 44%, and 65% higher
             risk of myocardial infarction, urgent revascularization, and
             stent thrombosis respectively when compared with
             unfractionated heparin with or without GpIIb/IIIa inhibitor.
             However, bivalirudin was associated with a 48% lower risk of
             major bleeding compared with unfractionated heparin plus
             GpIIb/IIIa inhibitor and 32% lower compared with
             unfractionated heparin alone.<h4>Conclusions</h4>In patients
             undergoing primary PCI, unfractionated heparin plus
             GpIIb/IIIa inhibitor and LMWH plus GpIIb/IIIa inhibitor were
             most efficacious, with the lowest rate of major adverse
             cardiovascular events, whereas bivalirudin was safest, with
             the lowest bleeding. These relationships should be
             considered in selecting anticoagulant therapies in patients
             undergoing primary PCI.},
   Doi = {10.1136/bmj.g6419},
   Key = {fds347535}
}

@article{fds347529,
   Author = {Nair, V and Sharma, D and Sahni, AK and Grover, N and Shankar, S and Jaiswal, SS and Dalal, SS and Basannar, DR and Phutane, VS and Kotwal,
             A and Gopal Rao and G and Batura, D and Venkatesh, MD and Sinha, T and Kumar,
             S and Joshi, DP},
   Title = {Antimicrobial use and antimicrobial resistance in nosocomial
             pathogens at a tertiary care hospital in
             Pune.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {71},
   Number = {2},
   Pages = {112-119},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.mjafi.2014.12.024},
   Abstract = {<h4>Background</h4>Resistance to antimicrobial agents is
             emerging in wide variety of nosocomial and community
             acquired pathogens. Widespread and often inappropriate use
             of broad spectrum antimicrobial agents is recognized as a
             significant contributing factor to the development and
             spread of bacterial resistance. This study was conducted to
             gain insight into the prevalent antimicrobial prescribing
             practices, and antimicrobial resistance pattern in
             nosocomial pathogens at a tertiary care hospital in Pune,
             India.<h4>Methods</h4>Series of one day cross sectional
             point prevalence surveys were carried out on four days
             between March and August 2014. All eligible in patients were
             included in the study. A structured data entry form was used
             to collect the data for each patient. Relevant samples were
             collected for microbiological examination from all the
             clinically identified hospital acquired infection
             cases.<h4>Results</h4>41.73% of the eligible patients (95%
             CI: 39.52-43.97) had been prescribed at least one
             antimicrobial during their stay in the hospital.
             Beta-lactams (38%) were the most prescribed antimicrobials,
             followed by Protein synthesis inhibitors (24%). Majority of
             the organisms isolated from Hospital acquired infection (HAI
             cases) were found to be resistant to the commonly used
             antimicrobials viz: Cefotaxime, Ceftriaxone, Amikacin,
             Gentamicin and Monobactams.<h4>Conclusion</h4>There is need
             to have regular antimicrobial susceptibility surveillance
             and dissemination of this information to the clinicians. In
             addition, emphasis on the rational use of antimicrobials,
             antimicrobial rotation and strict adherence to the standard
             treatment guidelines is very essential.},
   Doi = {10.1016/j.mjafi.2014.12.024},
   Key = {fds347529}
}

@article{fds346172,
   Author = {Sarkar, P and Biswas, D and Sindhwani, G and Rawat, J and Kotwal, A and Kakati, B},
   Title = {Application of lipoarabinomannan antigen in tuberculosis
             diagnostics: current evidence.},
   Journal = {Postgraduate medical journal},
   Volume = {90},
   Number = {1061},
   Pages = {155-163},
   Year = {2014},
   Month = {March},
   url = {http://dx.doi.org/10.1136/postgradmedj-2013-132053},
   Abstract = {Tests based on the detection of mycobacterial
             lipoarabinomannan (LAM) antigen in urine have emerged as
             potential point-of-care tests for tuberculosis (TB). We
             aimed to assimilate the current evidence regarding the
             diagnostic performance of LAM assays and to ascertain their
             clinical indication in settings with high and low prevalence
             of HIV-TB co-infection. Owing to suboptimal sensitivity, the
             urinary LAM assays are unsuitable as general screening tests
             for TB. However, unlike traditional diagnostic methods, they
             demonstrate improved sensitivity in HIV-TB co-infection
             which further increases with low CD4 counts. Accordingly,
             these assays are indicated as rule-in tests for TB in
             patients with advanced HIV-induced immunosuppression, and
             facilitate the early initiation of antituberculous treatment
             in them. They also offer incremental sensitivity and
             specificity when used as adjunct tests to smear microscopy
             and chest radiography in HIV-TB co-infection. They obviate
             the biohazards associated with sputum samples and provide an
             alternative diagnostic tool in sputum-scarce patients.
             Notwithstanding these advantages, the specificity of these
             assays is variable, which is mostly attributable to
             misclassification bias and cross-reactivity with
             non-tuberculous mycobacteria or other commensal flora.
             Furthermore, the inability to detect low titres of antigen
             in HIV-uninfected patients makes these assays unsuitable for
             use in settings with a low HIV prevalence. Future research
             targeted towards inclusion of specific monoclonal antibodies
             and more sensitive immunoassay platforms might help to
             improve the diagnostic performance of these assays and
             extend their applicability to the general population of
             patients with TB.},
   Doi = {10.1136/postgradmedj-2013-132053},
   Key = {fds346172}
}

@article{fds347533,
   Author = {Kotwal, A and Biswas, D and Kakati, B and Roy, S and Chauhan,
             BS},
   Title = {Aspergillus nidulans causing primary cutaneous aspergillosis
             in an immunocompetent patient.},
   Journal = {Cutis},
   Volume = {95},
   Number = {1},
   Pages = {E1-E3},
   Year = {2015},
   Month = {January},
   Key = {fds347533}
}

@article{fds356564,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA and Pereira,
             RA},
   Title = {ATLAS b-jet identification performance and efficiency
             measurement with tt¯ events in pp collisions at √s=13
             TeV},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {11},
   Year = {2019},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7450-8},
   Abstract = {The algorithms used by the ATLAS Collaboration during Run 2
             of the Large Hadron Collider to identify jets containing
             b-hadrons are presented. The performance of the algorithms
             is evaluated in the simulation and the efficiency with which
             these algorithms identify jets containing b-hadrons is
             measured in collision data. The measurement uses a
             likelihood-based method in a sample highly enriched in tt¯
             events. The topology of the t→ Wb decays is exploited to
             simultaneously measure both the jet flavour composition of
             the sample and the efficiency in a transverse momentum range
             from 20 to 600 GeV. The efficiency measurement is
             subsequently compared with that predicted by the simulation.
             The data used in this measurement, corresponding to a total
             integrated luminosity of 80.5 fb - 1, were collected in
             proton–proton collisions during the years 2015–2017 at a
             centre-of-mass energy s= 13 TeV. By simultaneously
             extracting both the efficiency and jet flavour composition,
             this measurement significantly improves the precision
             compared to previous results, with uncertainties ranging
             from 1 to 8% depending on the jet transverse
             momentum.},
   Doi = {10.1140/epjc/s10052-019-7450-8},
   Key = {fds356564}
}

@article{fds310336,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amaral
             Coutinho, Y and Amelung, C and Amor Dos Santos and SP and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov,
             A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B},
   Title = {ATLAS Collaboration},
   Journal = {Nuclear Physics A},
   Volume = {932},
   Pages = {572-594},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {December},
   url = {http://dx.doi.org/10.1016/S0375-9474(14)00601-0},
   Doi = {10.1016/S0375-9474(14)00601-0},
   Key = {fds310336}
}

@article{fds350339,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH},
   Title = {ATLAS data quality operations and performance for 2015-2018
             data-taking},
   Journal = {Journal of Instrumentation},
   Volume = {15},
   Number = {4},
   Year = {2020},
   Month = {April},
   url = {http://dx.doi.org/10.1088/1748-0221/15/04/P04003},
   Abstract = {The ATLAS detector at the Large Hadron Collider reads out
             particle collision data from over 100 million electronic
             channels at a rate of approximately 100 kHz, with a
             recording rate for physics events of approximately 1 kHz.
             Before being certified for physics analysis at computer
             centres worldwide, the data must be scrutinised to ensure
             they are clean from any hardware or software related issues
             that may compromise their integrity. Prompt identification
             of these issues permits fast action to investigate, correct
             and potentially prevent future such problems that could
             render the data unusable. This is achieved through the
             monitoring of detector-level quantities and reconstructed
             collision event characteristics at key stages of the data
             processing chain. This paper presents the monitoring and
             assessment procedures in place at ATLAS during 2015-2018
             data-taking. Through the continuous improvement of
             operational procedures, ATLAS achieved a high data quality
             efficiency, with 95.6% of the recorded proton-proton
             collision data collected at s=13 TeV certified for physics
             analysis.},
   Doi = {10.1088/1748-0221/15/04/P04003},
   Key = {fds350339}
}

@article{fds372327,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
             A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport, PP and Aloisio,
             A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev,
             V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
             Ferraz, V and Arcangeletti, C and Arce, ATH and Arena,
             E},
   Title = {ATLAS flavour-tagging algorithms for the LHC Run 2 pp
             collision dataset},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {7},
   Year = {2023},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11699-1},
   Abstract = {The flavour-tagging algorithms developed by the ATLAS
             Collaboration and used to analyse its dataset of s=13 TeV pp
             collisions from Run 2 of the Large Hadron Collider are
             presented. These new tagging algorithms are based on
             recurrent and deep neural networks, and their performance is
             evaluated in simulated collision events. These developments
             yield considerable improvements over previous jet-flavour
             identification strategies. At the 77% b-jet identification
             efficiency operating point, light-jet (charm-jet) rejection
             factors of 170 (5) are achieved in a sample of simulated
             Standard Model tt¯ events; similarly, at a c-jet
             identification efficiency of 30%, a light-jet (b-jet)
             rejection factor of 70 (9) is obtained.},
   Doi = {10.1140/epjc/s10052-023-11699-1},
   Key = {fds372327}
}

@article{fds307798,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {ATLAS measurements of the properties of jets for boosted
             particle searches},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.072006},
   Abstract = {Measurements are presented of the properties of high
             transverse momentum jets, produced in proton-proton
             collisions at a center-of-mass energy of √s=7TeV. The data
             correspond to an integrated luminosity of 35pb -1 and were
             collected with the ATLAS detector in 2010. Jet mass, width,
             eccentricity, planar flow and angularity are measured for
             jets reconstructed using the anti-kt algorithm with distance
             parameters R=0.6 and 1.0, with transverse momentum pT>300GeV
             and pseudorapidity |η|<2. The measurements are compared to
             the expectations of Monte Carlo generators that match
             leading-logarithmic parton showers to leading-order, or
             next-to-leading-order, matrix elements. The generators
             describe the general features of the jets, although
             discrepancies are observed in some distributions. © 2012
             CERN, for the ATLAS Collaboration Published by the American
             Physical Society under the terms of the http://creativecommons.
             org/licenses/by/3.0/ Creative Commons Attribution 3.0
             License. Further distribution of this work must maintain
             attribution to the author(s) and the published article's
             title, journal citation, and DOI.},
   Doi = {10.1103/PhysRevD.86.072006},
   Key = {fds307798}
}

@article{fds346168,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas,
             K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
             C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
             MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
             N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black,
             CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T},
   Title = {ATLAS Run 1 searches for direct pair production of
             third-generation squarks at the Large Hadron
             Collider.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {10},
   Pages = {510},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3726-9},
   Abstract = {This paper reviews and extends searches for the direct pair
             production of the scalar supersymmetric partners of the top
             and bottom quarks in proton-proton collisions collected by
             the ATLAS collaboration during the LHC Run 1. Most of the
             analyses use 20 [Formula: see text] of collisions at a
             centre-of-mass energy of [Formula: see text] TeV, although
             in some case an additional [Formula: see text] of collision
             data at [Formula: see text] TeV are used. New analyses are
             introduced to improve the sensitivity to specific regions of
             the model parameter space. Since no evidence of
             third-generation squarks is found, exclusion limits are
             derived by combining several analyses and are presented in
             both a simplified model framework, assuming simple decay
             chains, as well as within the context of more elaborate
             phenomenological supersymmetric models.},
   Doi = {10.1140/epjc/s10052-015-3726-9},
   Key = {fds346168}
}

@article{fds307661,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {ATLAS search for a heavy gauge boson decaying to a charged
             lepton and a neutrino in pp collisions at √s =7
             TeV},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {12},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2241-5},
   Abstract = {The ATLAS detector at the LHC is used to search for
             high-mass states, such as heavy charged gauge bosons (Wʹ),
             decaying to a charged lepton (electron or muon) and a
             neutrino. Results are presented based on the analysis of pp
             collisions at a center-of-mass energy of 7 TeV corresponding
             to an integrated luminosity of 4.7 fb−1. No excess beyond
             Standard Model expectations is observed. AWʹ with
             Sequential Standard Model couplings is excluded at the 95%
             credibility level for masses up to 2.55 TeV. Excited chiral
             bosons (W*) with equivalent coupling strength are excluded
             for masses up to 2.42 TeV.},
   Doi = {10.1140/epjc/s10052-012-2241-5},
   Key = {fds307661}
}

@article{fds317300,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {ATLAS search for new phenomena in dijet mass and angular
             distributions using pp collisions at √s = 7
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2013)029},
   Abstract = {Mass and angular distributions of dijets produced in LHC
             proton-proton collisions at a centre-of-mass energy √s =
             7TeV have been studied with the ATLAS detector using the
             full 2011 data set with an integrated luminosity of 4.8
             fb-1. Dijet masses up to ~ 4.0TeV have been probed. No
             resonance-like features have been observed in the dijet mass
             spectrum, and all angular distributions are consistent with
             the predictions of QCD. Exclusion limits on six hypotheses
             of new phenomena have been set at 95% CL in terms of mass or
             energy scale, as appropriate. These hypotheses include
             excited quarks below 2.83 TeV, colour octet scalars below
             1.86TeV, heavy W bosons below 1.68 TeV, string resonances
             below 3.61 TeV, quantum black holes with six extra
             space-time dimensions for quantum gravity scales below 4.11
             TeV, and quark contact interactions below a compositeness
             scale of 7.6 TeV in a destructive interference
             scenario.},
   Doi = {10.1007/JHEP01(2013)029},
   Key = {fds317300}
}

@article{fds362443,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
             SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury,
             KA and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari,
             N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C},
   Title = {AtlFast3: The Next Generation of Fast Simulation in
             ATLAS},
   Journal = {Computing and Software for Big Science},
   Volume = {6},
   Number = {1},
   Year = {2022},
   Month = {December},
   url = {http://dx.doi.org/10.1007/s41781-021-00079-7},
   Abstract = {The ATLAS experiment at the Large Hadron Collider has a
             broad physics programme ranging from precision measurements
             to direct searches for new particles and new interactions,
             requiring ever larger and ever more accurate datasets of
             simulated Monte Carlo events. Detector simulation with
             Geant4 is accurate but requires significant CPU resources.
             Over the past decade, ATLAS has developed and utilized tools
             that replace the most CPU-intensive component of the
             simulation—the calorimeter shower simulation—with faster
             simulation methods. Here, AtlFast3, the next generation of
             high-accuracy fast simulation in ATLAS, is introduced.
             AtlFast3 combines parameterized approaches with
             machine-learning techniques and is deployed to meet current
             and future computing challenges, and simulation needs of the
             ATLAS experiment. With highly accurate performance and
             significantly improved modelling of substructure within
             jets, AtlFast3 can simulate large numbers of events for a
             wide range of physics processes.},
   Doi = {10.1007/s41781-021-00079-7},
   Key = {fds362443}
}

@article{fds374561,
   Author = {ATLAS Collaboration},
   Title = {Author Correction: A detailed map of Higgs boson
             interactions by the ATLAS experiment ten years after the
             discovery.},
   Journal = {Nature},
   Volume = {623},
   Number = {7985},
   Pages = {E5},
   Year = {2023},
   Month = {November},
   url = {http://dx.doi.org/10.1038/s41586-023-06248-5},
   Doi = {10.1038/s41586-023-06248-5},
   Key = {fds374561}
}

@article{fds346179,
   Author = {Gupta, SK and Kotwal, J and Kotwal, A and Dhall, A and Garg,
             S},
   Title = {Authors' response.},
   Journal = {The Indian journal of medical research},
   Volume = {138},
   Number = {4},
   Pages = {562-563},
   Year = {2013},
   Month = {October},
   Key = {fds346179}
}

@article{fds323670,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arduini, G and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Beam-induced and cosmic-ray backgrounds observed in the
             ATLAS detector during the LHC 2012 proton-proton running
             period},
   Journal = {Journal of Instrumentation},
   Volume = {11},
   Number = {5},
   Pages = {P05013-P05013},
   Publisher = {IOP Publishing},
   Year = {2016},
   Month = {May},
   url = {http://dx.doi.org/10.1088/1748-0221/11/05/P05013},
   Abstract = {This paper discusses various observations on beam-induced
             and cosmic-ray backgrounds in the ATLAS detector during the
             LHC 2012 proton-proton run. Building on published results
             based on 2011 data, the correlations between background and
             residual pressure of the beam vacuum are revisited. Ghost
             charge evolution over 2012 and its role for backgrounds are
             evaluated. New methods to monitor ghost charge with beam-gas
             rates are presented and observations of LHC abort gap
             population by ghost charge are discussed in detail. Fake
             jets from colliding bunches and from ghost charge are
             analysed with improved methods, showing that ghost charge in
             individual radio-frequency buckets of the LHC can be
             resolved. Some results of two short periods of dedicated
             cosmic-ray background data-taking are shown; in particular
             cosmic-ray muon induced fake jet rates are compared to Monte
             Carlo simulations and to the fake jet rates from beam
             background. A thorough analysis of a particular LHC fill,
             where abnormally high background was observed, is presented.
             Correlations between backgrounds and beam intensity losses
             in special fills with very high β∗ are
             studied.},
   Doi = {10.1088/1748-0221/11/05/P05013},
   Key = {fds323670}
}

@article{fds308168,
   Author = {Hossenfelder, S and Bleicher, M and Hofmann, S and Stöcker, H and Kotwal, AV},
   Title = {Black hole relics in large extra dimensions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {566},
   Number = {3-4},
   Pages = {233-239},
   Publisher = {Elsevier BV},
   Year = {2003},
   Month = {July},
   url = {http://dx.doi.org/10.1016/S0370-2693(03)00835-9},
   Abstract = {Recent calculations applying statistical mechanics indicate
             that in a setting with compactified large extra dimensions a
             black hole might evolve into a (quasi-)stable state with
             mass close to the new fundamental scale Mf. Black holes and
             therefore their relics might be produced at the LHC in the
             case of extra-dimensional topologies. In this energy regime,
             Hawking's evaporation scenario is modified due to energy
             conservation and quantum effects. We reanalyse the
             evaporation of small black holes including the quantisation
             of the emitted radiation due to the finite surface of the
             black hole. It is found that observable stable black hole
             relics with masses ∼ 1-3Mf would form which could be
             identified by a delayed single jet with a corresponding hard
             momentum kick to the relic and by ionisation, e.g., in a
             TPC. © 2003 Published by Elsevier B.V.},
   Doi = {10.1016/S0370-2693(03)00835-9},
   Key = {fds308168}
}

@article{fds346176,
   Author = {Singh, R and Prakash, M and Dubey, R and Roy, K and Kotwal, A and Mahen,
             A},
   Title = {Body composition parameters as correlates of coronary artery
             disease.},
   Journal = {The Indian journal of medical research},
   Volume = {138},
   Number = {6},
   Pages = {1016-1019},
   Year = {2013},
   Month = {December},
   Abstract = {<h4>Background & objectives</h4>Obesity is a major risk
             factor for cardiovascular disease (CAD). This study was
             aimed to assess the risk for CAD determined by certain new
             and conventional body composition parameters such as
             visceral fat area (VFA), body mass index (BMI), waist to hip
             ratio (WHR), etc.<h4>Methods</h4>We did an age and sex
             matched case-control study of acute myocardial infarction
             with 100 participants in a tertiary care hospital (50 cases
             and 50 controls) representing the serving army personnel.
             The relation between VFA, per cent body fat (PBF), BMI,
             waist and hip circumferences, and WHR to CAD was
             assessed.<h4>Results</h4>The study showed that there was a
             significantly increased risk for CAD associated with VFA
             (OR: 5.67; 95% CI: 1.96, 16.95), WHR (7.07; 2.19, 24.27),
             waist circumference (WC) (2.63; 1.05, 6.66) and BMI (2.53;
             1.03, 6.26).<h4>Interpretation & conclusions</h4>In
             conclusion, increased VFA, BMI, WHR and WC showed an
             association with CAD. VFA is a good index for assessing not
             only visceral fat accumulation but also cardiovascular risk
             factors.},
   Key = {fds346176}
}

@article{fds374028,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
             W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
             AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung,
             C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH},
   Title = {Calibration of the light-flavour jet mistagging efficiency
             of the b-tagging algorithms with Z+jets events using 139 fb
             - 1 of ATLAS proton–proton collision data at
             √s=13 TeV},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {8},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11736-z},
   Abstract = {The identification of b-jets, referred to as b-tagging, is
             an important part of many physics analyses in the ATLAS
             experiment at the Large Hadron Collider and an accurate
             calibration of its performance is essential for high-quality
             physics results. This publication describes the calibration
             of the light-flavour jet mistagging efficiency in a data
             sample of proton–proton collision events at s=13 TeV
             corresponding to an integrated luminosity of 139 fb - 1 .
             The calibration is performed in a sample of Z bosons
             produced in association with jets. Due to the low mistagging
             efficiency for light-flavour jets, a method which uses
             modified versions of the b-tagging algorithms referred to as
             flip taggers is used in this work. A fit to the
             jet-flavour-sensitive secondary-vertex mass is performed to
             extract a scale factor from data, to correct the
             light-flavour jet mistagging efficiency in Monte Carlo
             simulations, while simultaneously correcting the b-jet
             efficiency. With this procedure, uncertainties coming from
             the modeling of jets from heavy-flavour hadrons are
             considerably lower than in previous calibrations of the
             mistagging scale factors, where they were dominant. The
             scale factors obtained in this calibration are consistent
             with unity within uncertainties.},
   Doi = {10.1140/epjc/s10052-023-11736-z},
   Key = {fds374028}
}

@article{fds308166,
   Author = {Affolder, T and Allspach, D and Ambrose, D and Bialek, J and Bokhari, W and Brozovic, M and Binkley, M and Burkett, K and Byon Wagner and A and Cogswell, F and Dressnandt, N and Feng, Z and Franklin, M and Galtieri,
             L and Gerdes, DW and Greenwood, J and Guarino, V and Guimaraes, J and da
             Costa, R and Haggerty, C},
   Title = {CDF Central Outer Tracker},
   Journal = {Nuclear Instruments and Methods in Physics Research Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {526},
   Number = {3},
   Pages = {249-299},
   Publisher = {Elsevier BV},
   Year = {2004},
   Month = {July},
   url = {http://dx.doi.org/10.1016/j.nima.2004.02.020},
   Abstract = {The Central Outer Tracker is a large cylindrical drift
             chamber constructed to replace Collider Detector at
             Fermilab's original central drift chamber for the higher
             luminosity expected for Run 2 at the Fermilab Tevatron. The
             chamber's drift properties are described in the context of
             meeting the operating requirements for Run 2. The design and
             construction of the chamber, the front- end readout
             electronics, and the high-voltage system are described in
             detail. Wire aging considerations are also
             discussed.},
   Doi = {10.1016/j.nima.2004.02.020},
   Key = {fds308166}
}

@article{fds310117,
   Author = {Baranovski, A and Benjamin, D and Cooper, G and Farrington, S and Genser, K and Hou, S and Hsieh, T and Kotwal, A and Lipeles, E and Murat,
             P and Norman, M and Robson, A and Sfiligoi, I and Snider, R and Stelzer, B and Syu, J and Timm, S and Vataga, E and Wolbers, S and Zhang,
             D},
   Title = {CDF II Production Farm Project},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {572},
   Number = {1 SPEC. ISS.},
   Pages = {399-401},
   Publisher = {Elsevier BV},
   Year = {2007},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.nima.2006.11.048},
   Abstract = {We describe the architecture and discuss our operational
             experience in running the off-line reconstruction farm of
             the CDFII experiment. The Linux PC-based farm performs a
             wide set of tasks, ranging from producing calibrations and
             primary event reconstruction to large scale ntuple
             production. The farm control software uses a standard Condor
             toolkit [The Condor project page, 〈http://www.cs.wisc.edu/condor〉]
             and the data handling part is based on SAM (Sequential
             Access via Metadata [Sequential data Access via Meta-data
             〈http://d0db.fnal.gov/sam/〉]) software. During its
             lifetime, the CDFII experiment will integrate a large amount
             of data (several petabytes) and the data processing chain is
             one of the key components of the successful physics program
             of the experiment. © 2006 Elsevier B.V. All rights
             reserved.},
   Doi = {10.1016/j.nima.2006.11.048},
   Key = {fds310117}
}

@article{fds310260,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Centrality and rapidity dependence of inclusive jet
             production in √sNN =5 .02 TeV proton–lead collisions
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {748},
   Pages = {392-413},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.07.023},
   Abstract = {Measurements of the centrality and rapidity dependence of
             inclusive jet production in sNN=5.02 TeV proton–lead
             (p+Pb) collisions and the jet cross-section in s=2.76 TeV
             proton–proton collisions are presented. These quantities
             are measured in datasets corresponding to an integrated
             luminosity of 27.8 nb−1 and 4.0 pb−1, respectively,
             recorded with the ATLAS detector at the Large Hadron
             Collider in 2013. The p+Pb collision centrality was
             characterised using the total transverse energy measured in
             the pseudorapidity interval −4.9 <η <−3.2 in the
             direction of the lead beam. Results are presented for the
             double-differential per-collision yields as a function of
             jet rapidity and transverse momentum (pT) for minimum-bias
             and centrality-selected p+Pb collisions, and are compared to
             the jet rate from the geometric expectation. The total jet
             yield in minimum-bias events is slightly enhanced above the
             expectation in a pT-dependent manner but is consistent with
             the expectation within uncertainties. The ratios of jet
             spectra from different centrality selections show a strong
             modification of jet production at all pT at forward
             rapidities and for large pT at mid-rapidity, which manifests
             as a suppression of the jet yield in central events and an
             enhancement in peripheral events. These effects imply that
             the factorisation between hard and soft processes is
             violated at an unexpected level in proton–nucleus
             collisions. Furthermore, the modifications at forward
             rapidities are found to be a function of the total jet
             energy only, implying that the violations may have a simple
             dependence on the hard parton–parton kinematics.},
   Doi = {10.1016/j.physletb.2015.07.023},
   Key = {fds310260}
}

@article{fds315923,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Centrality, rapidity, and transverse momentum dependence of
             isolated prompt photon production in lead-lead collisions at
             sNN =2.76 TeV measured with the ATLAS detector},
   Journal = {Physical Review C},
   Volume = {93},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {March},
   ISSN = {2469-9985},
   url = {http://dx.doi.org/10.1103/PhysRevC.93.034914},
   Abstract = {Prompt photon production in sNN=2.76-TeV Pb+Pb collisions
             has been measured by the ATLAS experiment at the Large
             Hadron Collider using data collected in 2011 with an
             integrated luminosity of 0.14 nb-1. Inclusive photon yields,
             scaled by the mean nuclear thickness function, are presented
             as a function of collision centrality and transverse
             momentum in two pseudorapidity intervals, |η|<1.37 and
             1.52≤|η|<2.37. The scaled yields in the two
             pseudorapidity intervals, as well as the ratios of the
             forward yields to those at midrapidity, are compared to the
             expectations from next-to-leading-order perturbative QCD
             (pQCD) calculations. The measured cross sections agree well
             with the predictions for proton-proton collisions within
             statistical and systematic uncertainties. Both the yields
             and the ratios are also compared to two other pQCD
             calculations, one which uses the isospin content appropriate
             to colliding lead nuclei and another which includes nuclear
             modifications to the nucleon parton distribution
             functions.},
   Doi = {10.1103/PhysRevC.93.034914},
   Key = {fds315923}
}

@article{fds316848,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
             S},
   Title = {Characterisation and mitigation of beam-induced backgrounds
             observed in the ATLAS detector during the 2011 proton-proton
             run},
   Journal = {Journal of Instrumentation},
   Volume = {8},
   Number = {7},
   Pages = {P07004-P07004},
   Publisher = {IOP Publishing},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1748-0221/8/07/P07004},
   Abstract = {This paper presents a summary of beam-induced backgrounds
             observed in the ATLAS detector and discusses methods to tag
             and remove background contaminated events in data.
             Triggerrate based monitoring of beam-related backgrounds is
             presented. The correlations of backgrounds with machine
             conditions, such as residual pressure in the beam-pipe, are
             discussed. Results from dedicated beam-background
             simulations are shown, and their qualitative agreement with
             data is evaluated. Data taken during the passage of
             unpaired, i.e. non-colliding, proton bunches is used to
             obtain background-enriched data samples. These are used to
             identify characteristic features of beam-induced
             backgrounds, which then are exploited to develop dedicated
             background tagging tools. These tools, based on observables
             in the Pixel detector, the muon spectrometer and the
             calorimeters, are described in detail and their efficiencies
             are evaluated. Finally an example of an application of these
             techniques to a monojet analysis is given, which
             demonstrates the importance of such event cleaning
             techniques for some new physics searches.},
   Doi = {10.1088/1748-0221/8/07/P07004},
   Key = {fds316848}
}

@article{fds321096,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel,
             C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro,
             LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
             K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund,
             OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan,
             AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel,
             O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
             MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister,
             I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio,
             D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez,
             SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana,
             S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
             A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El
             Moursli, RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A},
   Title = {Charged-particle distributions at low transverse momentum in
             [Formula: see text] TeV pp interactions measured
             with the ATLAS detector at the LHC.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {9},
   Pages = {502},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4335-y},
   Abstract = {Measurements of distributions of charged particles produced
             in proton-proton collisions with a centre-of-mass energy of
             13 TeV are presented. The data were recorded by the ATLAS
             detector at the LHC and correspond to an integrated
             luminosity of 151 [Formula: see text]. The particles are
             required to have a transverse momentum greater than 100 MeV
             and an absolute pseudorapidity less than 2.5. The
             charged-particle multiplicity, its dependence on transverse
             momentum and pseudorapidity and the dependence of the mean
             transverse momentum on multiplicity are measured in events
             containing at least two charged particles satisfying the
             above kinematic criteria. The results are corrected for
             detector effects and compared to the predictions from
             several Monte Carlo event generators.},
   Doi = {10.1140/epjc/s10052-016-4335-y},
   Key = {fds321096}
}

@article{fds321118,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
             R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi,
             S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier,
             S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
             TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN},
   Title = {Charged-particle distributions in pp interactions at
             [Formula: see text] measured with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {7},
   Pages = {403},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4203-9},
   Abstract = {This paper presents measurements of distributions of charged
             particles which are produced in proton-proton collisions at
             a centre-of-mass energy of [Formula: see text] and recorded
             by the ATLAS detector at the LHC. A special dataset recorded
             in 2012 with a small number of interactions per beam
             crossing (below 0.004) and corresponding to an integrated
             luminosity of 160 [Formula: see text] was used. A
             minimum-bias trigger was utilised to select a data sample of
             more than 9 million collision events. The multiplicity,
             pseudorapidity, and transverse momentum distributions of
             charged particles are shown in different regions of
             kinematics and charged-particle multiplicity, including
             measurements of final states at high multiplicity. The
             results are corrected for detector effects and are compared
             to the predictions of various Monte Carlo event generator
             models which simulate the full hadronic final
             state.},
   Doi = {10.1140/epjc/s10052-016-4203-9},
   Key = {fds321118}
}

@article{fds315919,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
   Title = {Charged-particle distributions in √s=13 TeV pp
             interactions measured with the ATLAS detector at the
             LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {758},
   Pages = {67-88},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {July},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.04.050},
   Abstract = {Charged-particle distributions are measured in
             proton–proton collisions at a centre-of-mass energy of 13
             TeV, using a data sample of nearly 9 million events,
             corresponding to an integrated luminosity of 170 μb−1,
             recorded by the ATLAS detector during a special Large Hadron
             Collider fill. The charged-particle multiplicity, its
             dependence on transverse momentum and pseudorapidity and the
             dependence of the mean transverse momentum on the
             charged-particle multiplicity are presented. The
             measurements are performed with charged particles with
             transverse momentum greater than 500 MeV and absolute
             pseudorapidity less than 2.5, in events with at least one
             charged particle satisfying these kinematic requirements.
             Additional measurements in a reduced phase space with
             absolute pseudorapidity less than 0.8 are also presented, in
             order to compare with other experiments. The results are
             corrected for detector effects, presented as particle-level
             distributions and are compared to the predictions of various
             Monte Carlo event generators.},
   Doi = {10.1016/j.physletb.2016.04.050},
   Key = {fds315919}
}

@booklet{Abbott97,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
             V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
             C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and di Loreto, G and Draper,
             P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {Color coherent radiation in multijet events from
             pp- collisions at √s = 1.8 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {414},
   Number = {3-4},
   Pages = {419-427},
   Publisher = {Elsevier BV},
   Year = {1997},
   Month = {November},
   url = {http://dx.doi.org/10.1016/S0370-2693(97)01190-8},
   Abstract = {We report on a study of color coherence effects in pp-
             collisions at a center of mass energy √s = 1.8 TeV. The
             data were collected with the DØ detector during the
             1992-1993 run of the Fermilab Tevatron Collider. We observe
             the presence of initial-to-final state color interference
             with the spatial correlations between soft and hard jets in
             multijet events in the central and in forward pseudorapidity
             regions. The results are compared to Monte Carlo simulations
             with different color coherence implementations and to the
             predictions of script O sign(α3s) QCD calculations. © 1997
             Elsevier Science B.V.},
   Doi = {10.1016/S0370-2693(97)01190-8},
   Key = {Abbott97}
}

@article{fds307799,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Alvarez
             González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
             A and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Asman, B and Atkins, S and Atramentov, O and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
             T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barreto, J and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Belanger-Champagne, C and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
             SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bezzubov, VA and Bhatia, S and Bhatnagar, V and Bhatti, A and Bhat, PC and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Brooijmans, G and Bross, A and Brown, D and Brown, J and Brucken, E and Bu,
             XB},
   Title = {Combination of CDF and D0 measurements of the W boson
             helicity in top quark decays},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.071106},
   Abstract = {We report the combination of recent measurements of the
             helicity of the W boson from top quark decay by the CDF and
             D0 collaborations, based on data samples corresponding to
             integrated luminosities of 2.7-5.4fb -1 of pp̄ collisions
             collected during Run II of the Fermilab Tevatron collider.
             Combining measurements that simultaneously determine the
             fractions of W bosons with longitudinal (f 0) and
             right-handed (f +) helicities, we find f
             0=0.722±0.081[±0.062(stat)±0.052(syst)] and f
             +=-0.033±0.046[±0.034(stat)±0.031(syst)]. Combining
             measurements where one of the helicity fractions is fixed to
             the value expected in the standard model, we find f
             0=0.682±0. 057[±0.035(stat)±0.046(syst)] for fixed f +
             and f +=-0.015±0.035[±0.018(stat)±0.030(syst)] for fixed
             f 0. The results are consistent with standard model
             expectations. © 2012 American Physical Society.},
   Doi = {10.1103/PhysRevD.85.071106},
   Key = {fds307799}
}

@article{fds308163,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Acosta, D and Adams, DL and Adams, M and Affolder, T and Ahmed, SN and Akimoto, H and Akopian, A and Albrow, MG and Alexeev, GD and Alton, A and Alves, GA and Amaral, P and Ambrose, D and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arnoud, Y and Arisawa, T and Artikov, A and Asakawa, T and Avila, C and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Babintsev, VV and Babukhadia, L and Bacchetta, N and Bachacou, H and Bacon, TC and Baden,
             A and Badgett, W and Baffioni, S and Bailey, MW and Bailey, S and Baldin,
             B and Balm, PW and Banerjee, S and Barbaro, P and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Baroiant,
             S and Barone, M and Barreto, J and Bartlett, JF and Bassler, U and Bauer,
             D and Bauer, G and Bean, A and Beaudette, F and Bedeschi, F and Behari, S and Begel, M and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Belyaev, A and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Beri, SB and Bernardi, G and Bertram, I and Berryhill, J and Besson, A and Beuselinck, R and Bevensee, B and Bezzubov, VA and Bhat,
             PC and Bhatnagar, V and Bhattacharjee, M and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blazey, G and Blekman, F and Blessing, S and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Boehnlein, A and Bojko,
             NI},
   Title = {Combination of CDF and D0 results on the [Formula Presented]
             boson mass and width},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {70},
   Number = {9},
   Pages = {17},
   Publisher = {American Physical Society (APS)},
   Year = {2004},
   Month = {Fall},
   url = {http://dx.doi.org/10.1103/PhysRevD.70.092008},
   Abstract = {The results based on 1992–95 data (Run 1) from the CDF and
             D0 experiments on the measurements of the [Formula
             Presented] boson mass and width are presented, along with
             the combined results. We report a Tevatron collider average
             [Formula Presented]. We also report the Tevatron collider
             average of the directly measured [Formula Presented] boson
             width [Formula Presented]. We describe a new joint analysis
             of the direct [Formula Presented] mass and width
             measurements. Assuming the validity of the standard model,
             we combine the directly measured [Formula Presented] boson
             width with the width extracted from the ratio of [Formula
             Presented] and [Formula Presented] boson leptonic partial
             cross sections. This combined result for the Tevatron is
             [Formula Presented]. Finally, we use the measurements of the
             direct total [Formula Presented] width and the leptonic
             branching ratio to extract the leptonic partial width
             [Formula Presented]. © 2004 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.70.092008},
   Key = {fds308163}
}

@article{fds307577,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
             T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Guimaraes Da Costa and J and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Beecher, D and Begalli, M and Behari, S and Bellantoni,
             L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon,
             M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti,
             A and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Boudreau, J and Boveia,
             A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg,
             C and Bross, A and Brown, D and Brucken, E and Bu, XB and Budagov, J and Budd,
             HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P},
   Title = {Combination of CDF and D0 W-Boson mass measurements},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {5},
   Pages = {052018},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.052018},
   Abstract = {We summarize and combine direct measurements of the mass of
             the W boson in √s=1.96 TeV proton-antiproton collision
             data collected by CDF and D0 experiments at the Fermilab
             Tevatron Collider. Earlier measurements from CDF and D0 are
             combined with the two latest, more precise measurements: a
             CDF measurement in the electron and muon channels using data
             corresponding to 2.2 fb-1 of integrated luminosity, and a D0
             measurement in the electron channel using data corresponding
             to 4.3 fb-1 of integrated luminosity. The resulting Tevatron
             average for the mass of the W boson is M W=80387±16 MeV.
             Including measurements obtained in electron-positron
             collisions at LEP yields the most precise value of M
             W=80385±15 MeV. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.88.052018},
   Key = {fds307577}
}

@article{fds356706,
   Author = {Sirunyan, AM and Tumasyan, A and Adam, W and Ambrogi, F and Asilar, E and Bergauer, T and Brandstetter, J and Brondolin, E and Dragicevic, M and Erö, J and Escalante Del Valle and A and Flechl, M and Friedl, M and Frühwirth, R and Ghete, VM and Grossmann, J and Hrubec, J and Jeitler,
             M and König, A and Krammer, N and Krätschmer, I and Liko, D and Madlener,
             T and Mikulec, I and Pree, E and Rad, N and Rohringer, H and Schieck, J and Schöfbeck, R and Spanring, M and Spitzbart, D and Taurok, A and Waltenberger, W and Wittmann, J and Wulz, CE and Zarucki, M and Chekhovsky, V and Mossolov, V and Suarez Gonzalez and J and De Wolf and EA and Di Croce and D and Janssen, X and Lauwers, J and Van De Klundert and M and Van
             Haevermaet, H and Van Mechelen and P and Van Remortel and N and Abu Zeid,
             S and Blekman, F and D’hondt, J and De Bruyn and I and De Clercq and J and Deroover, K and Flouris, G and Lontkovskyi, D and Lowette, S and Marchesini, I and Moortgat, S and Moreels, L and Python, Q and Skovpen,
             K and Tavernier, S and Van Doninck and W and Van Mulders and P and Van Parijs,
             I and Beghin, D and Bilin, B and Brun, H and Clerbaux, B and De Lentdecker,
             G and Delannoy, H and Dorney, B and Fasanella, G and Favart, L and Goldouzian, R and Grebenyuk, A and Kalsi, AK and Lenzi, T and Luetic, J and Maerschalk, T and Marinov, A and Seva, T and Starling, E and Vander
             Velde, C and Vanlaer, P and Vannerom, D and Yonamine, R and Zenoni, F and Cornelis, T and Dobur, D and Fagot, A and Gul, M and Khvastunov, I and Poyraz, D and Roskas, C and Salva, S and Tytgat, M and Verbeke, W and Zaganidis, N and Bakhshiansohi, H},
   Title = {Combination of inclusive and differential tt¯ charge
             asymmetry measurements using ATLAS and CMS data at √s = 7
             and 8 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {4},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP04(2018)033},
   Abstract = {This paper presents combinations of inclusive and
             differential measurements of the charge asymmetry (AC) in
             top quark pair (tt) events with a lepton+jets signature by
             the ATLAS and CMS Collaborations, using data from LHC
             proton-proton collisions at centreof- mass energies of 7 and
             8TeV. The data correspond to integrated luminosities of
             about 5 and 20 fb–1for each experiment, respectively. The
             resulting combined LHC measurements of the inclusive charge
             asymmetry are ACLHC7= 0:005±0:007 (stat) ±0:006 (syst) at
             7TeV and ACLHC7= 0:0055 ± 0:0023 (stat) ± 0:0025 (syst) at
             8TeV. These values, as well as the combination of AC
             measurements as a function of the invariant mass of the
             [formula presented] system at 8TeV, are consistent with the
             respective standard model predictions.},
   Doi = {10.1007/JHEP04(2018)033},
   Key = {fds356706}
}

@article{fds307542,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
             T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
             R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
             D and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu,
             A},
   Title = {Combination of measurements of the top-quark pair production
             cross section from the Tevatron Collider},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.072001},
   Abstract = {We combine six measurements of the inclusive top-quark pair
             (tt̄) production cross section (σtt̄) from data collected
             with the CDF and D0 detectors at the Fermilab Tevatron with
             proton-antiproton collisions at s=1.96TeV. The data
             correspond to integrated luminosities of up to 8.8fb-1. We
             obtain a value of σtt̄=7.60±0.41pb for a top-quark mass
             of mt=172.5GeV. The contributions to the uncertainty are
             0.20 pb from statistical sources, 0.29 pb from systematic
             sources, and 0.21 pb from the uncertainty on the integrated
             luminosity. The result is in good agreement with the
             standard model expectation of 7.35-0.33+0.28pb at
             next-to-next-to-leading order and next-to-next-to leading
             logarithms in perturbative QCD. © 2014 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.89.072001},
   Key = {fds307542}
}

@article{fds356659,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Combination of searches for heavy resonances decaying into
             bosonic and leptonic final states using 36 fb-1 of
             proton-proton collision data at s =13 TeV with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {5},
   Year = {2018},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.052008},
   Abstract = {Searches for new heavy resonances decaying into different
             pairings of W, Z, or Higgs bosons, as well as directly into
             leptons, are presented using a data sample corresponding to
             36.1 fb-1 of pp collisions at s=13 TeV collected during 2015
             and 2016 with the ATLAS detector at the CERN Large Hadron
             Collider. Analyses selecting bosonic decay modes in the
             qqqq, ννqq, ℓνqq, ℓℓqq, ℓνℓν, ℓℓνν,
             ℓνℓℓ, ℓℓℓℓ, qqbb, ννbb, ℓνbb, and
             ℓℓbb final states are combined, searching for a
             narrow-width resonance. Likewise, analyses selecting the
             leptonic ℓν and ℓℓ final states are also combined.
             These two sets of analyses are then further combined. No
             significant deviation from the Standard Model predictions is
             observed. Three benchmark models are tested: a model
             predicting the existence of a new heavy scalar singlet, a
             simplified model predicting a heavy vector-boson triplet,
             and a bulk Randall-Sundrum model with a heavy spin-2
             Kaluza-Klein excitation of the graviton. Cross section
             limits are set at the 95% confidence level using an
             asymptotic approximation and are compared with predictions
             for the benchmark models. These limits are also expressed in
             terms of constraints on couplings of the heavy vector-boson
             triplet to quarks, leptons, and the Higgs boson. The data
             exclude a heavy vector-boson triplet with mass below 5.5 TeV
             in a weakly coupled scenario and 4.5 TeV in a strongly
             coupled scenario, as well as a Kaluza-Klein graviton with
             mass below 2.3 TeV.},
   Doi = {10.1103/PhysRevD.98.052008},
   Key = {fds356659}
}

@article{fds356546,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
             Pereira, R},
   Title = {Combination of searches for Higgs boson pairs in pp
             collisions at s=13TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {800},
   Year = {2020},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.135103},
   Abstract = {This letter presents a combination of searches for Higgs
             boson pair production using up to 36.1 fb−1 of
             proton–proton collision data at a centre-of-mass energy
             s=13 TeV recorded with the ATLAS detector at the LHC. The
             combination is performed using six analyses searching for
             Higgs boson pairs decaying into the bb¯bb¯, bb¯W+W−,
             bb¯τ+τ−, W+W−W+W−, bb¯γγ and W+W−γγ final
             states. Results are presented for non-resonant and resonant
             Higgs boson pair production modes. No statistically
             significant excess in data above the Standard Model
             predictions is found. The combined observed (expected) limit
             at 95% confidence level on the non-resonant Higgs boson pair
             production cross-section is 6.9 (10) times the predicted
             Standard Model cross-section. Limits are also set on the
             ratio (κλ) of the Higgs boson self-coupling to its
             Standard Model value. This ratio is constrained at 95%
             confidence level in observation (expectation) to
             −5.0<κλ<12.0 (−5.8<κλ<12.0). In addition, limits are
             set on the production of narrow scalar resonances and spin-2
             Kaluza–Klein Randall–Sundrum gravitons. Exclusion
             regions are also provided in the parameter space of the
             habemus Minimal Supersymmetric Standard Model and the
             Electroweak Singlet Model.},
   Doi = {10.1016/j.physletb.2019.135103},
   Key = {fds356546}
}

@article{fds372126,
   Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
             J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
             W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
             PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
             Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
             V and Arcangeletti, C and Arce, ATH},
   Title = {Combination of searches for invisible decays of the Higgs
             boson using 139 fb−1 of proton-proton collision
             data at s=13 TeV collected with the ATLAS
             experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {842},
   Year = {2023},
   Month = {July},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.137963},
   Abstract = {Many extensions of the Standard Model predict the production
             of dark matter particles at the LHC. Sufficiently light dark
             matter particles may be produced in decays of the Higgs
             boson that would appear invisible to the detector. This
             Letter presents a statistical combination of searches for
             H→invisible decays where multiple production modes of the
             Standard Model Higgs boson are considered. These searches
             are performed with the ATLAS detector using 139 fb−1 of
             proton–proton collisions at a centre–of–mass energy of
             [Formula presented] at the LHC. In combination with the
             results at [Formula presented] and [Formula presented], an
             upper limit on the H→invisible branching ratio of 0.107
             (0.077) at the 95% confidence level is observed (expected).
             These results are also interpreted in the context of models
             where the 125 GeV Higgs boson acts as a portal to dark
             matter, and limits are set on the scattering cross-section
             of weakly interacting massive particles and
             nucleons.},
   Doi = {10.1016/j.physletb.2023.137963},
   Key = {fds372126}
}

@article{fds347443,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
             Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
             NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli,
             E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Arduh,
             FA and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster,
             AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azoulay, AM and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey,
             AJ and Bailey, VR and Baines, JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek,
             P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay,
             A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Bates, RL and Batista, SJ and Batlamous, S and Batley, JR and Batool,
             B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
             A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Besson,
             N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bi,
             R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bitadze, A and Bittrich, C and Bjergaard, DM and Black,
             JE and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
             AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borecka-Bielska, HM and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
             PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Bugge, MK and Bührer, F and Bulekov, O and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burr, JTP and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carter, JWS and Casado, MP and Casha, AF and Casper, DW and Castelijn,
             R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, B and Chen,
             C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Chu, MC and Chudoba, J},
   Title = {Combination of Searches for Invisible Higgs Boson Decays
             with the ATLAS Experiment.},
   Journal = {Physical review letters},
   Volume = {122},
   Number = {23},
   Pages = {231801},
   Year = {2019},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.122.231801},
   Abstract = {Dark matter particles, if sufficiently light, may be
             produced in decays of the Higgs boson. This Letter presents
             a statistical combination of searches for H→invisible
             decays where H is produced according to the standard model
             via vector boson fusion, Z(ℓℓ)H, and W/Z(had)H, all
             performed with the ATLAS detector using 36.1  fb^{-1} of
             pp collisions at a center-of-mass energy of
             sqrt[s]=13  TeV at the LHC. In combination with the
             results at sqrt[s]=7 and 8 TeV, an exclusion limit on the
             H→invisible branching ratio of 0.26(0.17_{-0.05}^{+0.07})
             at 95% confidence level is observed (expected).},
   Doi = {10.1103/physrevlett.122.231801},
   Key = {fds347443}
}

@article{fds307580,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Combination of searches for the Higgs boson using the full
             CDF data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.052013},
   Abstract = {We present a combination of searches for the standard model
             Higgs boson using the full CDF run II data set, which
             corresponds to an integrated luminosity of 9.45-10.0 fb-1
             collected from √s=1.96 TeV pp̄ collisions at the Fermilab
             Tevatron. The searches consider Higgs boson production from
             gluon-gluon fusion, vector-boson fusion, and associated
             production with either a W or Z boson or a tt̄ pair.
             Depending on the production mode, Higgs boson decays to
             W+W-, ZZ, bb̄, τ+τ-, and γγ are examined. We search for
             a Higgs boson with masses (mH) in the range 90-200 GeV/c2.
             In the absence of a signal, we expect based on combined
             search sensitivity to exclude at the 95% credibility level
             the mass regions 90<mH<94 GeV/c2, 96<mH<106 GeV/c2, and
             153<mH<175 GeV/c2. The observed exclusion regions are
             90<mH<102 GeV/c2 and 149<mH<172 GeV/c2. A moderate excess of
             signal-like events relative to the background expectation at
             the level of 2.0 standard deviations is present in the data
             for the mH=125 GeV/c2 search hypothesis. We also present
             interpretations of the data within the context of a
             fermiophobic model and an alternative standard model
             incorporating a fourth generation of fermions. Finally, for
             the hypothesis of a new particle with mass 125 GeV/c2, we
             constrain the coupling strengths of the new particle to W±
             bosons, Z bosons, and fermions. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.88.052013},
   Key = {fds307580}
}

@article{fds356772,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Combination of searches for WW, WZ, and ZZ resonances in pp
             collisions at √s=8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {755},
   Pages = {285-305},
   Year = {2016},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.02.015},
   Abstract = {The ATLAS experiment at the CERN Large Hadron Collider has
             performed searches for new, heavy bosons decaying to WW, WZ
             and ZZ final states in multiple decay channels using 20.3
             fb−1 of pp collision data at s=8 TeV. In the current
             study, the results of these searches are combined to provide
             a more stringent test of models predicting heavy resonances
             with couplings to vector bosons. Direct searches for a
             charged diboson resonance decaying to WZ in the
             ℓνℓ′ℓ′ (ℓ=μ,e), ℓℓqq¯ ℓνqq¯ and fully
             hadronic final states are combined and upper limits on the
             rate of production times branching ratio to the WZ bosons
             are compared with predictions of an extended gauge model
             with a heavy W′ boson. In addition, direct searches for a
             neutral diboson resonance decaying to WW and ZZ in the
             ℓℓqq¯ ℓνqq¯ and fully hadronic final states are
             combined and upper limits on the rate of production times
             branching ratio to the WW and ZZ bosons are compared with
             predictions for a heavy, spin-2 graviton in an extended
             Randall–Sundrum model where the Standard Model fields are
             allowed to propagate in the bulk of the extra
             dimension.},
   Doi = {10.1016/j.physletb.2016.02.015},
   Key = {fds356772}
}

@article{fds307911,
   Author = {Aaltonen, and T, and others},
   Title = {Combination of Tevatron searches for the standard model
             Higgs boson in the $W^+W^-$ decay mode},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {6},
   Pages = {061802},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.061802},
   Abstract = {http://arxiv.org/abs/1001.4162},
   Doi = {10.1103/PhysRevLett.104.061802},
   Key = {fds307911}
}

@article{fds347456,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azoulay, AM and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines,
             JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi
             Gupta, D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee,
             S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
             G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous,
             S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall,
             A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
             M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bi, R and Bianchi, RMB and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black,
             JE and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock,
             I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni,
             A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
             MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard,
             CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, V and Buschmann, E and Bussey,
             P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera
             Urbán, S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace,
             N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
             S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili,
             B and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen, H and Chen, J and Chen,
             S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng,
             HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D},
   Title = {Combination of the Searches for Pair-Produced Vectorlike
             Partners of the Third-Generation Quarks at
             sqrt[s]=13  TeV with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {121},
   Number = {21},
   Pages = {211801},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.121.211801},
   Abstract = {A combination of the searches for pair-produced vectorlike
             partners of the top and bottom quarks in various decay
             channels (T→Zt/Wb/Ht, B→Zb/Wt/Hb) is performed using
             36.1  fb^{-1} of pp collision data at
             sqrt[s]=13  TeV with the ATLAS detector at the Large
             Hadron Collider. The observed data are found to be in good
             agreement with the standard model background prediction in
             all individual searches. Therefore, combined
             95% confidence-level upper limits are set on the production
             cross section for a range of vectorlike quark scenarios,
             significantly improving upon the reach of the individual
             searches. Model-independent limits are set assuming the
             vectorlike quarks decay to standard model particles. A
             singlet T is excluded for masses below 1.31 TeV and a
             singlet B is excluded for masses below 1.22 TeV. Assuming a
             weak isospin (T,B) doublet and |V_{Tb}|≪|V_{tB}|, T and B
             masses below 1.37 TeV are excluded.},
   Doi = {10.1103/physrevlett.121.211801},
   Key = {fds347456}
}

@article{fds307694,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Alvarez
             González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
             A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
             T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins,
             S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
             JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
             SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori,
             L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brown, J and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett,
             K},
   Title = {Combination of the top-quark mass measurements from the
             Tevatron collider},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {9},
   Pages = {092003},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.092003},
   Abstract = {The top quark is the heaviest known elementary particle,
             with a mass about 40 times larger than the mass of its
             isospin partner, the bottom quark. It decays almost 100% of
             the time to a W boson and a bottom quark. Using top-antitop
             pairs at the Tevatron proton-antiproton collider, the CDF
             and D0 Collaborations have measured the top quark's mass in
             different final states for integrated luminosities of up to
             5.8fb-1. This paper reports on a combination of these
             measurements that results in a more precise value of the
             mass than any individual decay channel can provide. It
             describes the treatment of the systematic uncertainties and
             their correlations. The mass value determined is
             173.18±0.56(stat)±0.75(syst)GeV or 173.18±0.94GeV, which
             has a precision of ±0.54%, making this the most precise
             determination of the top-quark mass. © 2012 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.86.092003},
   Key = {fds307694}
}

@article{fds352490,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abou Zeid and OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and AlKhoury, K and Alberghi,
             GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri,
             AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
             Bella, L and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {Combination of the W boson polarization measurements in top
             quark decays using ATLAS and CMS data at √s = 8
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {8},
   Year = {2020},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2020)051},
   Abstract = {The combination of measurements of the W boson polarization
             in top quark decays performed by the ATLAS and CMS
             collaborations is presented. The measurements are based on
             proton-proton collision data produced at the LHC at a
             centre-of-mass energy of 8 TeV, and corresponding to an
             integrated luminosity of about 20 fb−1 for each
             experiment. The measurements used events containing one
             lepton and having different jet multiplicities in the final
             state. The results are quoted as fractions of W bosons with
             longitudinal (F0), left-handed (FL), or right-handed (FR)
             polarizations. The resulting combined measurements of the
             polarization fractions are F0 = 0.693 ± 0.014 and FL =
             0.315 ± 0.011. The fraction FR is calculated from the
             unitarity constraint to be FR = −0.008 ± 0.007. These
             results are in agreement with the standard model predictions
             at next-to-next-to-leading order in perturbative quantum
             chromodynamics and represent an improvement in precision of
             25 (29)% for F0 (FL) with respect to the most precise single
             measurement. A limit on anomalous right-handed vector (VR),
             and left- and right-handed tensor (gL, gR) tWb couplings is
             set while fixing all others to their standard model values.
             The allowed regions are [−0.11, 0.16] for VR, [−0.08,
             0.05] for gL, and [−0.04, 0.02] for gR, at 95% confidence
             level. Limits on the corresponding Wilson coefficients are
             also derived. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP08(2020)051},
   Key = {fds352490}
}

@article{fds356603,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
             Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
             NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
             AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini,
             MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras,
             D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V},
   Title = {Combinations of single-top-quark production cross-section
             measurements and},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {5},
   Year = {2019},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2019)088},
   Abstract = {This paper presents the combinations of single-top-quark
             production cross-section measurements by the ATLAS and CMS
             Collaborations, using data from LHC proton-proton collisions
             at s = 7 and 8 TeV corresponding to integrated luminosities
             of 1.17 to 5.1 fb−1 at s = 7 TeV and 12.2 to 20.3 fb−1
             at s = 8 TeV. These combinations are performed per
             centre-of-mass energy and for each production mode:
             t-channel, tW, and s-channel. The combined t-channel
             cross-sections are 67.5 ± 5.7 pb and 87.7 ± 5.8 pb at s =
             7 and 8 TeV respectively. The combined tW cross-sections are
             16.3 ± 4.1 pb and 23.1 ± 3.6 pb at s = 7 and 8 TeV
             respectively. For the s-channel cross-section, the
             combination yields 4.9 ± 1.4 pb at s = 8 TeV. The square of
             the magnitude of the CKM matrix element Vtb multiplied by a
             form factor fLV is determined for each production mode and
             centre-of-mass energy, using the ratio of the measured
             cross-section to its theoretical prediction. It is assumed
             that the top-quark-related CKM matrix elements obey the
             relation |Vtd|, |Vts| ≪ |Vtb|. All the |fLVVtb|2
             determinations, extracted from individual ratios at s = 7
             and 8 TeV, are combined, resulting in |fLVVtb| = 1.02 ±
             0.04 (meas.) ± 0.02 (theo.). All combined measurements are
             consistent with their corresponding Standard Model
             predictions.[Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP05(2019)088},
   Key = {fds356603}
}

@article{fds356709,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Aushev, V and Aushev, Y and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
             JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
             SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brochmann,
             M and Brock, R and Bromberg, C and Bross, A and Brown, D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu, A and Calamba, A and Camacho-Pérez, E and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chakrabarti, S and Chan, KM and Chandra, A and Chapelain,
             A and Chapon, E and Chen, G and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Cihangir, S and Claes, D and Clark, A and Clarke, C and Clutter, J and Convery, ME and Conway, J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou,
             M-C and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and Cuth, J and Cutts, D and Das, A and d'Ascenzo, N and Datta, M and Davies, G and de Barbaro, P and de Jong, SJ and De La
             Cruz-Burelo and E and Déliot, F and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov, SP and D'Errico, M and Desai, S and Deterre, C and DeVaughan, K and Devoto, F and Di Canto and A and Di Ruzza,
             B and Diehl, HT and Diesburg, M and Ding, PF and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, M and Driutti,
             A and Drutskoy, A and Dubey, A and Dudko, LV and Duperrin, A and Dutt, S and Eads, M and Ebina, K and Edgar, R and Edmunds, D and Elagin, A and Ellison,
             J and Elvira, VD and Enari, Y and Erbacher, R and Errede, S and Esham, B and Evans, H and Evdokimov, A and Evdokimov, VN and Farrington, S and Fauré, A and Feng, L and Ferbel, T and Fernández Ramos and JP and Fiedler, F and Field, R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest, R and Fortner, M and Fox, H and Franc, J and Franklin, M and Freeman, JC and Frisch, H and Fuess, S and Funakoshi, Y and Galloni, C and Garbincius, PH and Garcia-Bellido, A and García-González, JA and Garfinkel, AF and Garosi, P and Gavrilov,
             V and Geng, W and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gogota, O and Gold, M and Goldin, D and Golossanov, A and Golovanov, G and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grannis, PD and Greder, S and Greenlee, H and Grenier, G and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Grünendahl, S and Grünewald, MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hahn, SR and Haley, J and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, M and Harel, A and Harr,
             RF and Harrington-Taber, T and Hatakeyama, K and Hauptman, JM and Hays,
             C and Hays, J and Head, T and Hebbeker, T and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De
             La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hildreth, MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen, B and Hogan, J and Hohlfeld, M and Holzbauer, JL and Hong, Z and Hopkins, W and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeon, EJ and Jeong, MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere,
             A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung,
             AW and Junk, TR and Juste, A and Kajfasz, E and Kambeitz, M and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kato, Y and Katsanos, I and Kaur, M and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava, A and Kharzheev, YN and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Kiselevich,
             I and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Kruse, M and Kuhr,
             T and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Laasanen, AT and Lammel, S and Lammers, S and Lancaster, M and Lannon,
             K and Latino, G and Lebrun, P and Lee, HS and Lee, JS and Lee, SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis, JD and Li, D and Li,
             H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Liu, H and Liu, Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lys, J and Lysak, R and Maciel, AKA and Madar, R and Madrak, R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G and Manousakis-Katsikakis, A and Mansour,
             J and Marchese, L and Margaroli, F and Marino, P and Martínez-Ortega,
             J and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McCarthy, R and McGivern, CL and McNulty, R and Mehta, A and Mehtala, P and Meijer, MM and Melnitchouk, A and Menezes, D and Mercadante, PG and Merkin, M and Mesropian, C and Meyer, A and Meyer, J and Miao, T and Miconi, F and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondal, NK and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Mulhearn, M and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nagy, E and Nakano, I and Napier, A and Narain, M and Nayyar, R},
   Title = {Combined Forward-Backward Asymmetry Measurements in
             Top-Antitop Quark Production at the Tevatron.},
   Journal = {Physical review letters},
   Volume = {120},
   Number = {4},
   Pages = {042001},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.120.042001},
   Abstract = {The CDF and D0 experiments at the Fermilab Tevatron have
             measured the asymmetry between yields of forward- and
             backward-produced top and antitop quarks based on their
             rapidity difference and the asymmetry between their decay
             leptons. These measurements use the full data sets collected
             in proton-antiproton collisions at a center-of-mass energy
             of sqrt[s]=1.96  TeV. We report the results of
             combinations of the inclusive asymmetries and their
             differential dependencies on relevant kinematic quantities.
             The combined inclusive asymmetry is A_{FB}^{tt[over
             ¯]}=0.128±0.025. The combined inclusive and differential
             asymmetries are consistent with recent standard model
             predictions.},
   Doi = {10.1103/physrevlett.120.042001},
   Key = {fds356709}
}

@article{fds356637,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
   Title = {Combined measurement of differential and total cross
             sections in the H → γγ and the H → ZZ → 4ℓ
             decay channels at s=13 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {786},
   Pages = {114-133},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.09.019},
   Abstract = {A combined measurement of differential and inclusive total
             cross sections of Higgs boson production is performed using
             36.1 fb−1 of 13 TeV proton–proton collision data
             produced by the LHC and recorded by the ATLAS detector in
             2015 and 2016. Cross sections are obtained from measured
             H→γγ and H→ZZ⁎→4ℓ event yields, which are
             combined taking into account detector efficiencies,
             resolution, acceptances and branching fractions. The total
             Higgs boson production cross section is measured to be
             57.0−5.9+6.0 (stat.) −3.3+4.0 (syst.) pb, in agreement
             with the Standard Model prediction. Differential
             cross-section measurements are presented for the Higgs boson
             transverse momentum distribution, Higgs boson rapidity,
             number of jets produced together with the Higgs boson, and
             the transverse momentum of the leading jet. The results from
             the two decay channels are found to be compatible, and their
             combination agrees with the Standard Model
             predictions.},
   Doi = {10.1016/j.physletb.2018.09.019},
   Key = {fds356637}
}

@article{fds375227,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
             SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
             CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arbiol
             Val, SJ and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Artoni,
             G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol,
             AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal,
             D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Baer, TM and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Baker, OK and Bakos, E and Bakshi Gupta and D and Balakrishnan, V and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barel, MZ and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau, T and Beaucamp, JY and Beauchemin, PH and Becherer, F and Bechtle, P and Beck,
             HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berrocal Guardia and A and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhalla, NK and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Biryukov, S and Bisanz, T and Bisceglie, E and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov,
             VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borissov, G and Bortoletto, D and Boscherini,
             D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
             JE and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton,
             D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost,
             E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
             PA and Brüers, B and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
             AR and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai,
             Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carducci, G and Carli, T and Carlino, G and Carlotto, JI and Carlson,
             BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos,
             F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castillo,
             FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cepaitis, V and Cerny, K and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
             Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
             J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
             A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM},
   Title = {Combined Measurement of the Higgs Boson Mass from the
             H→γγ and H→ZZ^{*}→4ℓ Decay Channels with the ATLAS
             Detector Using sqrt[s]=7, 8, and 13 TeV pp Collision
             Data.},
   Journal = {Physical review letters},
   Volume = {131},
   Number = {25},
   Pages = {251802},
   Year = {2023},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.131.251802},
   Abstract = {A measurement of the mass of the Higgs boson combining the
             H→ZZ^{*}→4ℓ and H→γγ decay channels is presented.
             The result is based on 140  fb^{-1} of proton-proton
             collision data collected by the ATLAS detector during LHC
             run 2 at a center-of-mass energy of 13 TeV combined with
             the run 1 ATLAS mass measurement, performed at
             center-of-mass energies of 7 and 8 TeV, yielding a Higgs
             boson mass of 125.11±0.09(stat)±0.06(syst)=125.11±0.11  GeV.
             This corresponds to a 0.09% precision achieved on this
             fundamental parameter of the Standard Model of particle
             physics.},
   Doi = {10.1103/physrevlett.131.251802},
   Key = {fds375227}
}

@article{fds310284,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
             C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
             MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
             N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM},
   Title = {Combined Measurement of the Higgs Boson Mass in pp
             Collisions at sqrt[s]=7 and 8 TeV with the ATLAS and CMS
             Experiments.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {19},
   Pages = {191803},
   Year = {2015},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.114.191803},
   Abstract = {A measurement of the Higgs boson mass is presented based on
             the combined data samples of the ATLAS and CMS experiments
             at the CERN LHC in the H→γγ and H→ZZ→4ℓ decay
             channels. The results are obtained from a simultaneous fit
             to the reconstructed invariant mass peaks in the two
             channels and for the two experiments. The measured masses
             from the individual channels and the two experiments are
             found to be consistent among themselves. The combined
             measured mass of the Higgs boson is m_{H}=125.09±0.21
             (stat)±0.11 (syst) GeV.},
   Doi = {10.1103/physrevlett.114.191803},
   Key = {fds310284}
}

@article{fds356547,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Akesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Alvarez Piqueras and D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
             V},
   Title = {Combined measurements of Higgs boson production and decay
             using up to 80 fb-1 of proton-proton collision
             data at √s =13 TeV collected with the ATLAS
             experiment},
   Journal = {Physical Review D},
   Volume = {101},
   Number = {1},
   Year = {2020},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.101.012002},
   Abstract = {Combined measurements of Higgs boson production cross
             sections and branching fractions are presented. The
             combination is based on the analyses of the Higgs boson
             decay modes H → γγ, ZZ∗, WW∗, τ τ, bb, μ μ,
             searches for decays into invisible final states, and on
             measurements of off-shell Higgs boson production. Up to 79.8
             fb-1 of proton-proton collision data collected at √ = 13
             TeV with the ATLAS detector are used. Results are presented
             for the gluon-gluon fusion and vector-boson fusion
             processes, and for associated production with vector bosons
             or top-quarks. The global signal strength is determined to
             be μ = 1.11-0.08+0.09. The combined measurement yields an
             observed (expected) significance for the vector-boson fusion
             production process of 6.5δ (5.3δ). Measurements in
             kinematic regions defined within the simplified template
             cross section framework are also shown. The results are
             interpreted in terms of modifiers applied to the Standard
             Model couplings of the Higgs boson to other particles, and
             are used to set exclusion limits on parameters in
             two-Higgs-doublet models and in the simplified minimal
             supersymmetric Standard Model. No significant deviations
             from Standard Model predictions are observed.},
   Doi = {10.1103/PhysRevD.101.012002},
   Key = {fds356547}
}

@article{fds310403,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
             ME and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci,
             A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
             A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
             ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
             P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington,
             S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
             S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeans, DT and Jeon, EJ and Jindariani, S and Jones,
             M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi,
             A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Tipton, P and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund,
             AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson,
             JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Combined search for the standard model Higgs boson decaying
             to a bb pair using the full CDF data set.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {11},
   Pages = {111802},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevlett.109.111802},
   Abstract = {We combine the results of searches for the standard model
             (SM) Higgs boson based on the full CDF Run II data set
             obtained from sqrt[s]=1.96  TeV pp collisions at the
             Fermilab Tevatron corresponding to an integrated luminosity
             of 9.45  fb(-1). The searches are conducted for Higgs
             bosons that are produced in association with a W or Z boson,
             have masses in the range 90-150  GeV/c(2), and decay
             into bb pairs. An excess of data is present that is
             inconsistent with the background prediction at the level of
             2.5 standard deviations (the most significant local excess
             is 2.7 standard deviations).},
   Doi = {10.1103/physrevlett.109.111802},
   Key = {fds310403}
}

@article{fds307720,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Combined search for the Standard Model Higgs boson in pp
             collisions at √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.032003},
   Abstract = {A combined search for the Standard Model Higgs boson with
             the ATLAS detector at the LHC is presented. The data sets
             used correspond to integrated luminosities from 4.6fb-1 to
             4.9fb-1 of proton-proton collisions collected at √s=7TeV
             in 2011. The Higgs boson mass ranges of 111.4 GeV to 116.6
             GeV, 119.4 GeV to 122.1 GeV, and 129.2 GeV to 541 GeV are
             excluded at the 95% confidence level, while the range 120
             GeV to 560 GeV is expected to be excluded in the absence of
             a signal. An excess of events is observed at Higgs boson
             mass hypotheses around 126 GeV with a local significance of
             2.9 standard deviations (σ). The global probability for the
             background to produce an excess at least as significant
             anywhere in the entire explored Higgs boson mass range of
             110-600 GeV is estimated to be ∼15%, corresponding to a
             significance of approximately 1σ. © 2012
             CERN.},
   Doi = {10.1103/PhysRevD.86.032003},
   Key = {fds307720}
}

@article{fds307778,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Combined search for the Standard Model Higgs boson using up
             to 4.9 fb-1 of pp collision data at s=7TeV with
             the ATLAS detector at the LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {710},
   Number = {1},
   Pages = {49-66},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.044},
   Abstract = {A combined search for the Standard Model Higgs boson with
             the ATLAS experiment at the LHC using datasets corresponding
             to integrated luminosities from 1.04 fb-1 to 4.9 fb-1 of pp
             collisions collected at s=7TeV is presented. The Higgs boson
             mass ranges 112.9-115.5 GeV, 131-238 GeV and 251-466 GeV are
             excluded at the 95% confidence level (CL), while the range
             124-519 GeV is expected to be excluded in the absence of a
             signal. An excess of events is observed around mH~126GeV
             with a local significance of 3.5 standard deviations (σ).
             The local significances of H→γγ, H→ZZ(z.ast;)→ℓ+ℓ-ℓ'+ℓ'-
             and H→WW(z.ast;)→ℓ+νℓ'-ν- the three most sensitive
             channels in this mass range, are 2.8σ, 2.1σ and 1.4σ,
             respectively. The global probability for the background to
             produce such a fluctuation anywhere in the explored Higgs
             boson mass range 110-600 GeV is estimated to be ~1.4% or,
             equivalently, 2.2σ. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.02.044},
   Key = {fds307778}
}

@article{fds307914,
   Author = {Aaltonen, and T, and others},
   Title = {Combined Tevatron upper limit on $gg\rightarrow{}H\rightarrow{}W^{+}W^{-}$
             and constraints on the Higgs boson mass in fourth-generation
             fermion models},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {1},
   Pages = {011102},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.011102},
   Abstract = {We combine results from searches by the CDF and D0
             collaborations for a standard model Higgs boson (H) in the
             process gg→H→W+W - in pp̄ collisions at the Fermilab
             Tevatron Collider at √s=1.96TeV. With 4.8fb-1 of
             integrated luminosity analyzed at CDF and 5.4fb-1 at D0, the
             95% confidence level upper limit on σ(gg→H)×B(H→W+W-)
             is 1.75 pb at mH=120GeV, 0.38 pb at mH=165GeV, and 0.83 pb
             at mH=200GeV. Assuming the presence of a fourth sequential
             generation of fermions with large masses, we exclude at the
             95% confidence level a standard-model-like Higgs boson with
             a mass between 131 and 204 GeV. © 2010 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.82.011102},
   Key = {fds307914}
}

@article{fds346216,
   Author = {Seth, T and Kotwal, A and Thakur, R and Singh, P and Kochupillai,
             V},
   Title = {Common cancers in India: knowledge, attitudes and behaviours
             of urban slum dwellers in New Delhi.},
   Journal = {Public health},
   Volume = {119},
   Number = {2},
   Pages = {87-96},
   Year = {2005},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.puhe.2004.05.013},
   Abstract = {<h4>Research questions</h4>What is the level of knowledge
             and awareness of common cancers? What are the prevalent
             attitudes and behaviours relating to common
             cancers?<h4>Objectives</h4>To assess knowledge, attitudes
             and behaviours regarding common cancers amongst urban slum
             dwellers in New Delhi.<h4>Study design</h4>Field-based
             cross-sectional survey of an urban slum cluster.<h4>Setting</h4>Slum
             clusters along Pankha Road, West New Delhi.<h4>Participants</h4>Slum
             dwellers of selected slums.<h4>Study variables</h4>Independent
             variables were sociodemographic factors. Dependent variables
             were knowledge, attitudes and behaviours regarding
             preventive and curative aspects of common
             cancers.<h4>Statistical analysis</h4>Proportions, confidence
             intervals, tests of significance and multiple logistic
             regression.<h4>Results</h4>Only 13% (10.6-15.7%) of the
             study participants were aware of Pap smears, and only 2%
             (1.1-3.3%) were able to identify all the common signs of
             cancer. However, 87% (84.4-89.5%) of the study participants
             knew that tobacco is a risk factor for cancer. Overall, 51%
             (47.2-54.7%) had some knowledge pertaining to
             cancer.<h4>Conclusion</h4>A focused, concerted and effective
             information, education and communication drive is urgently
             needed for all aspects of common cancers in
             India.},
   Doi = {10.1016/j.puhe.2004.05.013},
   Key = {fds346216}
}

@article{fds347537,
   Author = {Vasilopoulos, T and Kotwal, A and Huisingh-Scheetz, MJ and Waite, LJ and McClintock, MK and Dale, W},
   Title = {Comorbidity and chronic conditions in the National Social
             Life, Health and Aging Project (NSHAP), Wave
             2.},
   Journal = {The journals of gerontology. Series B, Psychological
             sciences and social sciences},
   Volume = {69 Suppl 2},
   Pages = {S154-S165},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1093/geronb/gbu025},
   Abstract = {<h4>Objective</h4>The goals of this paper were: (a) to
             promote research using the National Social Life, Health and
             Aging Project (NSHAP) Wave 2 data by providing relevant
             background information for a broad range of chronic
             conditions and (b) to provide a framework for combining
             these chronic conditions into informative comorbidity
             indices.<h4>Method</h4>The chronic conditions measured in
             NSHAP Wave 2 were grouped across several health domains:
             cardiovascular, endocrine and metabolic, cancer, lung,
             inflammatory and bone, neurological, and sensorimotor.
             Prevalences for each condition were reported as percentages
             and were also estimated separately by age group and gender.
             Additionally, 2 comorbidity indices were created: a Modified
             Charlson Comorbidity Index (CCI) that included conditions
             associated with mortality risk and the NSHAP Comorbidity
             Index (NCI) that included conditions from the Modified CCI
             as well as additional conditions related to overall health
             and function.<h4>Results</h4>Hypertension, incontinence,
             arthritis, heart conditions, cancer, and diabetes were the
             most prevalent conditions. In general, prevalences of most
             chronic conditions increased with age. Additionally, there
             were several notable gender differences in chronic condition
             prevalence. Due to the inclusion of highly prevalent
             conditions, such as hypertension and incontinence, the mean
             comorbidity index score of the NCI was higher than that of
             the Modified CCI.<h4>Discussion</h4>Wave 2 of NSHAP included
             a variety of measures assessing the chronic conditions that
             are the most prevalent in older adults. These data are a
             valuable resource for the study of the impact of chronic
             conditions on overall health and aging.},
   Doi = {10.1093/geronb/gbu025},
   Key = {fds347537}
}

@article{fds356633,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik,
             Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Pereira, RA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold,
             H},
   Title = {Comparison between simulated and observed LHC beam
             backgrounds in the ATLAS experiment at E beam =4
             TeV},
   Journal = {Journal of Instrumentation},
   Volume = {13},
   Number = {12},
   Year = {2018},
   Month = {December},
   url = {http://dx.doi.org/10.1088/1748-0221/13/12/P12006},
   Abstract = {Results of dedicated Monte Carlo simulations of beam-induced
             background (BIB) in the ATLAS experiment at the Large Hadron
             Collider (LHC) are presented and compared with data recorded
             in 2012. During normal physics operation this background
             arises mainly from scattering of the 4 TeV protons on
             residual gas in the beam pipe. Methods of reconstructing the
             BIB signals in the ATLAS detector, developed and implemented
             in the simulation chain based on the \textsc{Fluka} Monte
             Carlo simulation package, are described. The interaction
             rates are determined from the residual gas pressure
             distribution in the LHC ring in order to set an absolute
             scale on the predicted rates of BIB so that they can be
             compared quantitatively with data. Through these comparisons
             the origins of the BIB leading to different observables in
             the ATLAS detectors are analysed. The level of agreement
             between simulation results and BIB measurements by ATLAS in
             2012 demonstrates that a good understanding of the origin of
             BIB has been reached.},
   Doi = {10.1088/1748-0221/13/12/P12006},
   Key = {fds356633}
}

@article{fds347183,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
             M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
             E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
             M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
             KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
             U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
             D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
             BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
             S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V},
   Title = {Comparison of Fragmentation Functions for Jets Dominated by
             Light Quarks and Gluons from pp and Pb+Pb Collisions in
             ATLAS.},
   Journal = {Physical review letters},
   Volume = {123},
   Number = {4},
   Pages = {042001},
   Year = {2019},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.123.042001},
   Abstract = {Charged-particle fragmentation functions for jets
             azimuthally balanced by a high-transverse-momentum, prompt,
             isolated photon are measured in 25  pb^{-1} of pp and
             0.49  nb^{-1} of Pb+Pb collision data at 5.02 TeV per
             nucleon pair recorded with the ATLAS detector at the Large
             Hadron Collider. The measurements are compared to
             predictions of Monte Carlo generators and to measurements
             of inclusively selected jets. In pp collisions, a different
             jet fragmentation function in photon-tagged events from that
             in inclusive jet events arises from the difference in
             fragmentation between light quarks and gluons. The ratios of
             the fragmentation functions in Pb+Pb events to that in pp
             events are used to explore the parton color-charge
             dependence of jet quenching in the hot medium. In relatively
             peripheral collisions, fragmentation functions exhibit a
             similar modification pattern for photon-tagged and inclusive
             jets. However, photon-tagged jets are observed to have
             larger modifications than inclusive jets in central Pb+Pb
             events.},
   Doi = {10.1103/physrevlett.123.042001},
   Key = {fds347183}
}

@article{fds313622,
   Author = {Kotwal, AV and Jayatilaka, B},
   Title = {Comparison of HORACE and PHOTOS algorithms for multiphoton
             emission in the context of W boson mass measurement},
   Journal = {Advances in High Energy Physics},
   Volume = {2016},
   Number = {1615081},
   Pages = {1-9},
   Publisher = {Hindawi Limited},
   Year = {2016},
   Month = {January},
   ISSN = {1687-7357},
   url = {http://dx.doi.org/10.1155/2016/1615081},
   Abstract = {W boson mass measurement is sensitive to QED radiative
             corrections due to virtual photon loops and real photon
             emission. The largest shift in the measured mass, which
             depends on the transverse momentum spectrum of the charged
             lepton from the boson decay, is caused by the emission of
             real photons from the final-state lepton. There are a number
             of calculations and codes available to model the final-state
             photon emission. We perform a detailed study, comparing the
             results from horace and photos implementations of the
             final-state multiphoton emission in the context of a direct
             measurement of W boson mass at Tevatron. Mass fits are
             performed using a simulation of the CDF II
             detector.},
   Doi = {10.1155/2016/1615081},
   Key = {fds313622}
}

@article{fds373066,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
             J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
             Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
             GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
             M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
             JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
             C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
             KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
   Title = {Comparison of inclusive and photon-tagged jet suppression in
             5.02 TeV Pb+Pb collisions with ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {846},
   Year = {2023},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.138154},
   Abstract = {Parton energy loss in the quark–gluon plasma (QGP) is
             studied with a measurement of photon-tagged jet production
             in 1.7 nb−1 of Pb+Pb data and 260 pb−1 of pp data, both
             at sNN=5.02 TeV, with the ATLAS detector. The process pp
             →γ+jet+X and its analogue in Pb+Pb collisions is measured
             in events containing an isolated photon with transverse
             momentum (pT) above 50 GeV and reported as a function of jet
             pT. This selection results in a sample of jets with a
             steeply falling pT distribution that are mostly initiated by
             the showering of quarks. The pp and Pb+Pb measurements are
             used to report the nuclear modification factor, RAA, and the
             fractional energy loss, Sloss, for photon-tagged jets. In
             addition, the results are compared with the analogous ones
             for inclusive jets, which have a significantly smaller
             quark-initiated fraction. The RAA and Sloss values are found
             to be significantly different between those for
             photon-tagged jets and inclusive jets, demonstrating that
             energy loss in the QGP is sensitive to the colour-charge of
             the initiating parton. The results are also compared with a
             variety of theoretical models of colour-charge-dependent
             energy loss.},
   Doi = {10.1016/j.physletb.2023.138154},
   Key = {fds373066}
}

@article{fds310337,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Comprehensive measurements of t-channel single top-quark
             production cross sections at √s=7 TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.112006},
   Abstract = {This article presents measurements of the t-channel single
             top-quark (t) and top-antiquark (t¯) total production cross
             sections σ(tq) and σ(t¯q), their ratio
             Rt=σ(tq)/σ(t¯q), and a measurement of the inclusive
             production cross section σ(tq+t¯q) in proton-proton
             collisions at √s=7 TeV at the LHC. Differential cross
             sections for the tq and t¯q processes are measured as a
             function of the transverse momentum and the absolute value
             of the rapidity of t and t¯, respectively. The analyzed
             data set was recorded with the ATLAS detector and
             corresponds to an integrated luminosity of 4.59 fb-1.
             Selected events contain one charged lepton, large missing
             transverse momentum, and two or three jets. The cross
             sections are measured by performing a binned
             maximum-likelihood fit to the output distributions of neural
             networks. The resulting measurements are
             σ(tq)=46±1(stat)±6(syst) pb, σ(t¯q)=23±1(stat)±3(syst)
             pb, Rt=2.04±0.13(stat)±0.12(syst), and
             σ(tq+t¯q)=68±2(stat)±8(syst) pb, consistent with the
             Standard Model expectation. The uncertainty on the measured
             cross sections is dominated by systematic uncertainties,
             while the uncertainty on Rt is mainly statistical. Using the
             ratio of σ(tq+t¯q) to its theoretical prediction, and
             assuming that the top-quark-related CKM matrix elements obey
             the relation |Vtb||Vts|,|Vtd|, we determine
             |Vtb|=1.02±0.07.},
   Doi = {10.1103/PhysRevD.90.112006},
   Key = {fds310337}
}

@article{fds360566,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alison, J and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
             Bella, L and Aranzabal, N and Araujo Ferraz and V and Pereira, RA and Arcangeletti, C and Arce, ATH},
   Title = {Configuration and performance of the ATLAS b-jet triggers in
             Run 2},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {12},
   Year = {2021},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09775-5},
   Abstract = {Several improvements to the ATLAS triggers used to identify
             jets containing b-hadrons (b-jets) were implemented for
             data-taking during Run 2 of the Large Hadron Collider from
             2016 to 2018. These changes include reconfiguring the b-jet
             trigger software to improve primary-vertex finding and allow
             more stable running in conditions with high pile-up, and the
             implementation of the functionality needed to run
             sophisticated taggers used by the offline reconstruction in
             an online environment. These improvements yielded an order
             of magnitude better light-flavour jet rejection for the same
             b-jet identification efficiency compared to the performance
             in Run 1 (2011–2012). The efficiency to identify b-jets
             in the trigger, and the conditional efficiency for b-jets
             that satisfy offline b-tagging requirements to pass the
             trigger are also measured. Correction factors are derived to
             calibrate the b-tagging efficiency in simulation to match
             that observed in data. The associated systematic
             uncertainties are substantially smaller than in previous
             measurements. In addition, b-jet triggers were operated for
             the first time during heavy-ion data-taking, using dedicated
             triggers that were developed to identify semileptonic
             b-hadron decays by selecting events with geometrically
             overlapping muons and jets.},
   Doi = {10.1140/epjc/s10052-021-09775-5},
   Key = {fds360566}
}

@article{fds364959,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
             M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C and Arce, ATH and Arguin, JF},
   Title = {Constraints on Higgs boson properties using
             WW(→ eνμν) jj production in
             36.1fb-1 of √s=13 TeV pp collisions with the
             ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {82},
   Number = {7},
   Year = {2022},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-022-10366-1},
   Abstract = {This article presents the results of two studies of Higgs
             boson properties using the WW∗(→ eνμν) jj final
             state, based on a dataset corresponding to 36.1 fb - 1 of
             s=13 TeV proton–proton collisions recorded by the ATLAS
             experiment at the Large Hadron Collider. The first study
             targets Higgs boson production via gluon–gluon fusion and
             constrains the CP properties of the effective Higgs–gluon
             interaction. Using angular distributions and the overall
             rate, a value of tan (α) = 0.0 ± 0.4 (stat.) ± 0.3
             (syst.) is obtained for the tangent of the mixing angle for
             CP-even and CP-odd contributions. The second study exploits
             the vector-boson fusion production mechanism to probe the
             Higgs boson couplings to longitudinally and transversely
             polarised W and Z bosons in both the production and the
             decay of the Higgs boson; these couplings have not been
             directly constrained previously. The polarisation-dependent
             coupling-strength scale factors are defined as the ratios of
             the measured polarisation-dependent coupling strengths to
             those predicted by the Standard Model, and are determined
             using rate and kinematic information to be
             aL=0.91-0.18+0.10(stat.)-0.17+0.09(syst.) and aT= 1.2 ± 0.4
             (stat.)-0.3+0.2(syst.). These coupling strengths are
             translated into pseudo-observables, resulting in
             κVV=0.91-0.18+0.10(stat.)-0.17+0.09(syst.) and
             ϵVV=0.13-0.20+0.28 (stat.)-0.10+0.08(syst.). All results
             are consistent with the Standard Model predictions.},
   Doi = {10.1140/epjc/s10052-022-10366-1},
   Key = {fds364959}
}

@article{fds356607,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Arduh, FA},
   Title = {Constraints on mediator-based dark matter and scalar dark
             energy models using √s = 13 TeV pp collision data
             collected by the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {5},
   Year = {2019},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2019)142},
   Abstract = {Constraints on selected mediator-based dark matter models
             and a scalar dark energy model using up to 37 fb−1s = 13
             TeV pp collision data collected by the ATLAS detector at the
             LHC during 2015-2016 are summarised in this paper. The
             results of experimental searches in a variety of final
             states are interpreted in terms of a set of spin-1 and
             spin-0 single-mediator dark matter simplified models and a
             second set of models involving an extended Higgs sector plus
             an additional vector or pseudo-scalar mediator. The searches
             considered in this paper constrain spin-1 leptophobic and
             leptophilic mediators, spin-0 colour-neutral and
             colour-charged mediators and vector or pseudo-scalar
             mediators embedded in extended Higgs sector models. In this
             case, also s = 8 TeV pp collision data are used for the
             interpretation of the results. The results are also
             interpreted for the first time in terms of light scalar
             particles that could contribute to the accelerating
             expansion of the universe (dark energy).[Figure not
             available: see fulltext.].},
   Doi = {10.1007/JHEP05(2019)142},
   Key = {fds356607}
}

@article{fds310290,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo,
             N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Galloni, C and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn,
             SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes,
             RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori,
             M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
             JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
             M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
             G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
             A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
             P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese,
             L and Margaroli, F and Marino, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu,
             C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes,
             L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
             C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
             K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and (CDF
             Collaboration)},
   Title = {Constraints on models of the Higgs boson with exotic spin
             and parity using decays to bottom-antibottom quarks in the
             full CDF data set.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {14},
   Pages = {141802},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.114.141802},
   Abstract = {A search for particles with the same mass and couplings as
             those of the standard model Higgs boson but different spin
             and parity quantum numbers is presented. We test two
             specific alternative Higgs boson hypotheses: a pseudoscalar
             Higgs boson with spin-parity J^{P}=0^{-} and a gravitonlike
             Higgs boson with J^{P}=2^{+}, assuming for both a mass of
             125  GeV/c^{2}. We search for these exotic states
             produced in association with a vector boson and decaying
             into a bottom-antibottom quark pair. The vector boson is
             reconstructed through its decay into an electron or muon
             pair, or an electron or muon and a neutrino, or it is
             inferred from an imbalance in total transverse momentum. We
             use expected kinematic differences between events containing
             exotic Higgs bosons and those containing standard model
             Higgs bosons. The data were collected by the CDF experiment
             at the Tevatron proton-antiproton collider, operating at a
             center-of-mass energy of sqrt[s]=1.96  TeV, and
             correspond to an integrated luminosity of 9.45  fb^{-1}.
             We exclude deviations from the predictions of the standard
             model with a Higgs boson of mass 125  GeV/c^{2} at the
             level of 5 standard deviations, assuming signal strengths
             for exotic boson production equal to the prediction for the
             standard model Higgs boson, and set upper limits of
             approximately 30% relative to the standard model rate on the
             possible rate of production of each exotic
             state.},
   Doi = {10.1103/physrevlett.114.141802},
   Key = {fds310290}
}

@article{fds348986,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Constraints on new phenomena via Higgs boson couplings and
             invisible decays with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {11},
   Pages = {1-52},
   Year = {2015},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2015)206},
   Abstract = {Abstract: The ATLAS experiment at the LHC has measured the
             Higgs boson couplings and mass, and searched for invisible
             Higgs boson decays, using multiple production and decay
             channels with up to 4.7 fb−1 of pp collision data at−1at
             TeV. In the current study, the measured production and decay
             rates of the observed Higgs boson in the γγ, ZZ, W W ,
             Zγ, bb, τ τ , and μμ decay channels, along with results
             from the associated production of a Higgs boson with a
             top-quark pair, are used to probe the scaling of the
             couplings with mass. Limits are set on parameters in
             extensions of the Standard Model including a composite Higgs
             boson, an additional electroweak singlet, and
             two-Higgs-doublet models. Together with the measured mass of
             the scalar Higgs boson in the γγ and ZZ decay modes, a
             lower limit is set on the pseudoscalar Higgs boson mass of
             mA> 370 GeV in the “hMSSM” simplified Minimal
             Supersymmetric Standard Model. Results from direct searches
             for heavy Higgs bosons are also interpreted in the hMSSM.
             Direct searches for invisible Higgs boson decays in the
             vector-boson fusion and associated production of a Higgs
             boson with W/Z (Z → ℓℓ, W/Z → jj) modes are
             statistically combined to set an upper limit on the Higgs
             boson invisible branching ratio of 0.25. The use of the
             measured visible decay rates in a more general coupling fit
             improves the upper limit to 0.23, constraining a Higgs
             portal model of dark matter.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP11(2015)206},
   Key = {fds348986}
}

@article{fds356781,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Constraints on non-Standard Model Higgs boson interactions
             in an effective Lagrangian using differential cross sections
             measured in the H → γγ decay channel at √s=8 TeV with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {753},
   Pages = {69-85},
   Year = {2016},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.11.071},
   Abstract = {The strength and tensor structure of the Higgs boson's
             interactions are investigated using an effective Lagrangian,
             which introduces additional CP-even and CP-odd interactions
             that lead to changes in the kinematic properties of the
             Higgs boson and associated jet spectra with respect to the
             Standard Model. The parameters of the effective Lagrangian
             are probed using a fit to five differential cross sections
             previously measured by the ATLAS experiment in the H→γγ
             decay channel with an integrated luminosity of 20.3 fb−1
             at s=8 TeV. In order to perform a simultaneous fit to the
             five distributions, the statistical correlations between
             them are determined by re-analysing the H→γγ candidate
             events in the proton–proton collision data. No significant
             deviations from the Standard Model predictions are observed
             and limits on the effective Lagrangian parameters are
             derived. The statistical correlations are made publicly
             available to allow for future analysis of theories with
             non-Standard Model interactions.},
   Doi = {10.1016/j.physletb.2015.11.071},
   Key = {fds356781}
}

@article{fds356640,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {Constraints on off-shell Higgs boson production and the
             Higgs boson total width in ZZ → 4ℓ and
             ZZ → 2ℓ2ν final states with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {786},
   Pages = {223-244},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.09.048},
   Abstract = {A measurement of off-shell Higgs boson production in the
             ZZ→4ℓ and ZZ→2ℓ2ν decay channels, where ℓ stands
             for either an electron or a muon, is performed using data
             from proton–proton collisions at a centre-of-mass energy
             of s=13 TeV. The data were collected by the ATLAS experiment
             in 2015 and 2016 at the Large Hadron Collider, and they
             correspond to an integrated luminosity of 36.1fb−1. An
             observed (expected) upper limit on the off-shell Higgs
             signal strength, defined as the event yield normalised to
             the Standard Model prediction, of 3.8 (3.4) is obtained at
             95% confidence level (CL). Assuming the ratio of the Higgs
             boson couplings to the Standard Model predictions is
             independent of the momentum transfer of the Higgs production
             mechanism considered in the analysis, a combination with the
             on-shell signal-strength measurements yields an observed
             (expected) 95% CL upper limit on the Higgs boson total width
             of 14.4 (15.2) MeV.},
   Doi = {10.1016/j.physletb.2018.09.048},
   Key = {fds356640}
}

@article{fds371633,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
             CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
             P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
             C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev,
             V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
             JF},
   Title = {Constraints on spin-0 dark matter mediators and invisible
             Higgs decays using ATLAS 13 TeV pp collision data with two
             top quarks and missing transverse momentum in the final
             state},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {6},
   Year = {2023},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11477-z},
   Abstract = {This paper presents a statistical combination of searches
             targeting final states with two top quarks and invisible
             particles, characterised by the presence of zero, one or two
             leptons, at least one jet originating from a b-quark and
             missing transverse momentum. The analyses are searches for
             phenomena beyond the Standard Model consistent with the
             direct production of dark matter in pp collisions at the
             LHC, using 139 fb - 1 of data collected with the ATLAS
             detector at a centre-of-mass energy of 13 TeV. The results
             are interpreted in terms of simplified dark matter models
             with a spin-0 scalar or pseudoscalar mediator particle. In
             addition, the results are interpreted in terms of upper
             limits on the Higgs boson invisible branching ratio, where
             the Higgs boson is produced according to the Standard Model
             in association with a pair of top quarks. For scalar
             (pseudoscalar) dark matter models, with all couplings set to
             unity, the statistical combination extends the mass range
             excluded by the best of the individual channels by
             50 (25) GeV, excluding mediator masses up to 370 GeV. In
             addition, the statistical combination improves the expected
             coupling exclusion reach by 14% (24%), assuming a scalar
             (pseudoscalar) mediator mass of 10 GeV. An upper limit on
             the Higgs boson invisible branching ratio of 0.38
             (0.30-0.09+0.13) is observed (expected) at 95% confidence
             level.},
   Doi = {10.1140/epjc/s10052-023-11477-z},
   Key = {fds371633}
}

@article{fds372124,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
             SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Aly, M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
             CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
   Title = {Constraints on the Higgs boson self-coupling from single-
             and double-Higgs production with the ATLAS detector using pp
             collisions at s=13 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {843},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.137745},
   Abstract = {Constraints on the Higgs boson self-coupling are set by
             combining double-Higgs boson analyses in the bb¯bb¯,
             bb¯τ+τ− and bb¯γγ decay channels with single-Higgs
             boson analyses targeting the γγ, ZZ⁎, WW⁎, τ+τ−
             and bb¯ decay channels. The data used in these analyses
             were recorded by the ATLAS detector at the LHC in
             proton–proton collisions at s=13 TeV and correspond to an
             integrated luminosity of 126–139 fb−1. The combination
             of the double-Higgs analyses sets an upper limit of μHH<2.4
             at 95% confidence level on the double-Higgs production
             cross-section normalised to its Standard Model prediction.
             Combining the single-Higgs and double-Higgs analyses, with
             the assumption that new physics affects only the Higgs boson
             self-coupling (λHHH), values outside the interval
             −0.4<κλ=(λHHH/λHHHSM)<6.3 are excluded at 95%
             confidence level. The combined single-Higgs and double-Higgs
             analyses provide results with fewer assumptions, by adding
             in the fit more coupling modifiers introduced to account for
             the Higgs boson interactions with the other Standard Model
             particles. In this relaxed scenario, the constraint becomes
             −1.4<κλ<6.1 at 95% CL.},
   Doi = {10.1016/j.physletb.2023.137745},
   Key = {fds372124}
}

@article{fds310330,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Piqueras, DÁ and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
             C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
             MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
             N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
             S},
   Title = {Constraints on the off-shell Higgs boson signal strength in
             the high-mass ZZ and WW final states with the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {335},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3542-2},
   Abstract = {Measurements of the <i>ZZ</i> and <i>WW</i> final states in
             the mass range above the [Formula: see text] and [Formula:
             see text] thresholds provide a unique opportunity to measure
             the off-shell coupling strength of the Higgs boson. This
             paper presents constraints on the off-shell Higgs boson
             event yields normalised to the Standard Model prediction
             (signal strength) in the [Formula: see text], [Formula: see
             text] and [Formula: see text] final states. The result is
             based on <i>pp</i> collision data collected by the ATLAS
             experiment at the LHC, corresponding to an integrated
             luminosity of 20.3 fb[Formula: see text] at a collision
             energy of [Formula: see text] TeV. Using the [Formula: see
             text] method, the observed 95 [Formula: see text]
             confidence level (CL) upper limit on the off-shell signal
             strength is in the range 5.1-8.6, with an expected range of
             6.7-11.0. In each case the range is determined by varying
             the unknown [Formula: see text] and [Formula: see text]
             background K-factor from higher-order quantum chromodynamics
             corrections between half and twice the value of the known
             signal K-factor. Assuming the relevant Higgs boson couplings
             are independent of the energy scale of the Higgs boson
             production, a combination with the on-shell measurements
             yields an observed (expected) 95 [Formula: see text] CL
             upper limit on [Formula: see text] in the range 4.5-7.5
             (6.5-11.2) using the same variations of the background
             K-factor. Assuming that the unknown [Formula: see text]
             background K-factor is equal to the signal K-factor, this
             translates into an observed (expected) 95 [Formula: see
             text] CL upper limit on the Higgs boson total width of 22.7
             (33.0) MeV.},
   Doi = {10.1140/epjc/s10052-015-3542-2},
   Key = {fds310330}
}

@article{fds329965,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
             D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Armitage, LJ},
   Title = {Correction to: Identification and rejection of pile-up jets
             at high pseudorapidity with the ATLAS detector (Eur. Phys.
             J. C, (2017), 77, (580), 10.1140/epjc/s10052-017-5081-5)},
   Journal = {European Physical Journal C},
   Volume = {77},
   Number = {10},
   Publisher = {Springer Nature America, Inc},
   Year = {2017},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5245-3},
   Abstract = {Unfortunately, in the original version of this article the
             copyright holder was wrong in the HTML. The original article
             has been corrected.},
   Doi = {10.1140/epjc/s10052-017-5245-3},
   Key = {fds329965}
}

@article{fds356625,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {Correlated long-range mixed-harmonic fluctuations measured
             in pp, p+Pb and low-multiplicity Pb+Pb collisions with the
             ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {789},
   Pages = {444-471},
   Year = {2019},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.11.065},
   Abstract = {Correlations of two flow harmonics vn and vm via three- and
             four-particle cumulants are measured in 13 TeV pp, 5.02 TeV
             p+Pb, and 2.76 TeV peripheral Pb+Pb collisions with the
             ATLAS detector at the LHC. The goal is to understand the
             multi-particle nature of the long-range collective
             phenomenon in these collision systems. The large non-flow
             background from dijet production present in the standard
             cumulant method is suppressed using a method of subevent
             cumulants involving two, three and four subevents separated
             in pseudorapidity. The results show a negative correlation
             between v2 and v3 and a positive correlation between v2 and
             v4 for all collision systems and over the full multiplicity
             range. However, the magnitudes of the correlations are found
             to depend on the event multiplicity, the choice of
             transverse momentum range and collision system. The relative
             correlation strength, obtained by normalisation of the
             cumulants with the 〈vn2〉 from a two-particle correlation
             analysis, is similar in the three collision systems and
             depends weakly on the event multiplicity and transverse
             momentum. These results based on the subevent methods
             provide strong evidence of a similar long-range
             multi-particle collectivity in pp, p+Pb and peripheral Pb+Pb
             collisions.},
   Doi = {10.1016/j.physletb.2018.11.065},
   Key = {fds356625}
}

@article{fds346214,
   Author = {Kotwal, A and Thakur, R and Seth, T},
   Title = {Correlates of tobacco-use pattern amongst adolescents in two
             schools of New Delhi, India.},
   Journal = {Indian journal of medical sciences},
   Volume = {59},
   Number = {6},
   Pages = {243-252},
   Year = {2005},
   Month = {June},
   url = {http://dx.doi.org/10.4103/0019-5359.16299},
   Abstract = {<h4>Background</h4>As adolescent tobacco use has been found
             to be a major predictor of future use, preventive efforts
             need to be focused on this section of population.<h4>Objectives</h4>To
             assess the role of knowledge regarding tobacco, risk-taking
             attitude, peers, and other influencers on tobacco and areca
             nut use, amongst adolescents.<h4>Settings and design</h4>A
             school-based cross-sectional study covering two schools.
             Students of classes IX and XI, of selected schools,
             participated in the study (n = 596).<h4>Methods</h4>A
             pretested and validated, close ended, self-administered
             questionnaire was used. Sociodemographic factors, awareness
             regarding tobacco, risk-taking attitudes, role of peers and
             other influencers, and tobacco, areca nut and alcohol use,
             were studied.<h4>Statistical analysis</h4>Point estimates,
             98% Confidence Intervals, tests of significance, bivariate
             and multivariate analysis (multiple logistic
             regression).<h4>Results</h4>Almost 42% of tobacco users
             started before the age of 12 years. Peer pressure, general
             stress, and media were important influencers. Logistic
             regression analysis showed that students in public school
             were using more tobacco [Odds ratio (OR) = 1.85, P = 0.174]
             and tobacco/areca nut (OR = 1.14, P = 0.02). The difference
             in use between the genders and class in which studying was
             statistically not significant. Lesser proportion of those
             possessing adequate knowledge regarding tobacco used it as
             compared to those without adequate knowledge (OR = 0.13, P <
             0.001) however, possession of adequate knowledge was not a
             good predictor of areca nut consumption (OR = 0.86, P =
             0.585). The most important correlate for tobacco use (OR =
             6.41, P < 0.001) and areca nut use (OR = 11.17, P < 0.001)
             was risk-taking attitude.<h4>Conclusion</h4>Multi-pronged
             and concerted efforts targeting children at an early age are
             required to prevent tobacco and areca nut use among
             adolescents.},
   Doi = {10.4103/0019-5359.16299},
   Key = {fds346214}
}

@article{fds346184,
   Author = {Tiwari, M and Kotwal, J and Kotwal, A and Mishra, P and Dutta, V and Chopra, S},
   Title = {Correlation of haemoglobin and red cell indices with serum
             ferritin in Indian women in second and third trimester of
             pregnancy.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {69},
   Number = {1},
   Pages = {31-36},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.mjafi.2012.07.016},
   Abstract = {<h4>Background</h4>Iron deficiency anaemia (IDA) is the most
             common cause of anaemia in pregnancy in Indians and is
             associated with increased risk of low birth-weight infants.
             Studies from developed countries recommend iron
             supplementation based on serum ferritin levels. However,
             screening by serum ferritin is not feasible in all cases in
             India. This study was undertaken to document haematological
             profile of pregnant Indian women.<h4>Methods</h4>We studied
             the correlation between second and third trimester ferritin
             concentration and haemoglobin (Hb) and red cell indices in
             100 consecutive ANC cases to select the best haematologic
             characteristic to identify women who needed iron therapy. Hb
             and red cell indices, RBC count, mean corpuscular volume,
             mean corpuscular haemoglobin, mean corpuscular haemoglobin
             concentration, red cell distribution width were analysed and
             PBS studied to subtype anaemia if present.<h4>Results</h4>Proportion
             of iron deficiency anaemia in pregnancy was 34% and
             significant correlation was found between serum ferritin and
             RDW-CV% and TRBC. No correlation was found between ferritin
             levels and Hb, MCV, MCH and MCHC. Serum ferritin levels were
             <12 ng/mL in 30 out of 52 non-anaemic cases suggesting
             prevalence of sub-clinical iron deficiency in 58% cases.
             None of the red cell indices correlated with ferritin level
             in this group. Only TRBC showed some correlation with
             ferritin (r = -0.090, p > 0.05).<h4>Conclusion</h4>All
             pregnant women in India should continue to get iron
             supplements unlike what is recommended in the developed
             countries where iron supplementation is based on serum
             ferritin levels.},
   Doi = {10.1016/j.mjafi.2012.07.016},
   Key = {fds346184}
}

@article{fds372392,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
             CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
             MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei,
             D and Dos Santos and SPA and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
             JF},
   Title = {Correlations between flow and transverse momentum in Xe + Xe
             and Pb + Pb collisions at the LHC with the ATLAS detector: A
             probe of the heavy-ion initial state and nuclear
             deformation},
   Journal = {Physical Review C},
   Volume = {107},
   Number = {5},
   Year = {2023},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevC.107.054910},
   Abstract = {The correlations between flow harmonics vn for n = 2, 3, and
             4 and mean transverse momentum [pT] in 129Xe + 129Xe and
             208Pb + 208Pb collisions at √s = 5.44 and 5.02 TeV,
             respectively, are measured using charged particles with the
             ATLAS detector. The correlations are potentially sensitive
             to the shape and size of the initial geometry, nuclear
             deformation, and initial momentum anisotropy. The effects
             from nonflow and centrality fluctuations are minimized,
             respectively, via a subevent cumulant method and an
             event-activity selection based on particle production at
             very forward rapidity. The vn-[pT] correlations show strong
             dependencies on centrality, harmonic number n, pT, and
             pseudorapidity range. Current models qualitatively describe
             the overall centrality- and system-dependent trends but fail
             to quantitatively reproduce all features of the data. In
             central collisions, where models generally show good
             agreement, the v2-[pT] correlations are sensitive to the
             triaxiality of the quadruple deformation. Comparison of the
             model with the Pb + Pb and Xe + Xe data confirms that the
             129Xe nucleus is a highly deformed triaxial ellipsoid that
             has neither a prolate nor oblate shape. This provides strong
             evidence for a triaxial deformation of the 129Xe nucleus
             from high-energy heavy-ion collisions.},
   Doi = {10.1103/PhysRevC.107.054910},
   Key = {fds372392}
}

@article{fds351555,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asai,
             K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou,
             EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis,
             C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji,
             S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Besson,
             N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman,
             M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich,
             C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona,
             M and Bonilla, JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler,
             S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burr, JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba,
             LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carratta, G and Carter, JWS and Carter,
             TM and Casado, MP and Casha, AF and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
             DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen,
             J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng,
             HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chow, YS and Christopher, LD and Chu, MC and Chu, X},
   Title = {CP Properties of Higgs Boson Interactions with Top Quarks in
             the tt[over ¯]H and tH Processes Using H→γγ with the
             ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {125},
   Number = {6},
   Pages = {061802},
   Year = {2020},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.125.061802},
   Abstract = {A study of the charge conjugation and parity (CP) properties
             of the interaction between the Higgs boson and top quarks is
             presented. Higgs bosons are identified via the diphoton
             decay channel (H→γγ), and their production in
             association with a top quark pair (tt[over ¯]H) or single
             top quark (tH) is studied. The analysis uses
             139  fb^{-1} of proton-proton collision data recorded at
             a center-of-mass energy of sqrt[s]=13  TeV with the
             ATLAS detector at the Large Hadron Collider. Assuming a
             CP-even coupling, the tt[over ¯]H process is observed with
             a significance of 5.2 standard deviations. The measured
             cross section times H→γγ branching ratio is
             1.64_{-0.36}^{+0.38}(stat)_{-0.14}^{+0.17}(sys)  fb, and
             the measured rate for tt[over ¯]H is 1.43_{-0.31}^{+0.33}(stat)_{-0.15}^{+0.21}(sys)
             times the Standard Model expectation. The tH production
             process is not observed and an upper limit on its rate of 12
             times the Standard Model expectation is set. A CP-mixing
             angle greater (less) than 43 (-43)° is excluded at
             95% confidence level.},
   Doi = {10.1103/physrevlett.125.061802},
   Key = {fds351555}
}

@article{fds308208,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
             JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
             R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
             D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada,
             J},
   Title = {Cross section for b-jet production in supp¯p
             collisions at √s=1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {85},
   Number = {24},
   Pages = {5068-5073},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.85.5068},
   Abstract = {Bottom-quark production in p¯p collisions at √s=1.8 TeV
             is studied with 5 pb−1 of data collected in 1995 by the D0
             detector at the Fermilab Tevatron Collider. The differential
             production cross section for b jets in the central rapidity
             region (|yb|<1) as a function of jet transverse energy is
             extracted from a muon-tagged jet sample. Within experimental
             and theoretical uncertainties, D0 results are found to be
             higher than, but compatible with, next-to-leading-order QCD
             predictions. © 2000 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.85.5068},
   Key = {fds308208}
}

@article{fds356609,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {Cross-section measurements of the Higgs boson decaying into
             a pair of τ -leptons in proton-proton collisions at s =13
             TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {99},
   Number = {7},
   Year = {2019},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.99.072001},
   Abstract = {A measurement of production cross sections of the Higgs
             boson in proton-proton collisions is presented in the
             H→ττ decay channel. The analysis is performed using 36.1
             fb-1 of data recorded by the ATLAS experiment at the Large
             Hadron Collider at a center-of-mass energy of s=13 TeV. All
             combinations of leptonic (τ→vv with =e,μ) and hadronic
             (τ→hadrons v) τ decays are considered. The H→ττ
             signal over the expected background from other Standard
             Model processes is established with an observed (expected)
             significance of 4.4 (4.1) standard deviations. Combined with
             results obtained using data taken at 7 and 8 TeV
             center-of-mass energies, the observed (expected)
             significance amounts to 6.4 (5.4) standard deviations and
             constitutes an observation of H→ττ decays. Using the
             data taken at s=13 TeV, the total cross section in the
             H→ττ decay channel is measured to be 3.77-0.59+0.60
             (stat) -0.74+0.87 (syst) pb, for a Higgs boson of mass 125
             GeV assuming the relative contributions of its production
             modes as predicted by the Standard Model. Total cross
             sections in the H→ττ decay channel are determined
             separately for vector-boson-fusion production and
             gluon-gluon-fusion production to be σH→ττVBF=0.28±0.09
             (stat) -0.09+0.11 (syst) pb and σH→ττggF=3.1±1.0
             (stat) -1.3+1.6 (syst) pb, respectively. Similarly, results
             of a fit are reported in the framework of simplified
             template cross sections. All measurements are in agreement
             with Standard Model expectations.},
   Doi = {10.1103/PhysRevD.99.072001},
   Key = {fds356609}
}

@article{fds346204,
   Author = {Kotwal, A and Watt, D},
   Title = {Cutaneous squamous cell carcinoma in a child.},
   Journal = {Journal of plastic, reconstructive & aesthetic surgery :
             JPRAS},
   Volume = {62},
   Number = {7},
   Pages = {e194-e195},
   Year = {2009},
   Month = {July},
   url = {http://dx.doi.org/10.1016/j.bjps.2009.03.008},
   Abstract = {Cutaneous squamous cell carcinoma in children is very rare.
             Of those reported cases, most arise in the context of
             underlying predisposing conditions such as xeroderma
             pigmentosum, albinism or immunosuppression. We report a rare
             case of cutaneous squamous cell carcinoma in a child with no
             history of predisposing conditions.},
   Doi = {10.1016/j.bjps.2009.03.008},
   Key = {fds346204}
}

@article{fds321098,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Dark matter interpretations of ATLAS searches for the
             electroweak production of supersymmetric particles in √s=8
             TeV proton-proton collisions},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2016)175},
   Abstract = {A selection of searches by the ATLAS experiment at the LHC
             for the electroweak production of SUSY particles are used to
             study their impact on the constraints on dark matter
             candidates. The searches use 20 fb−1 of proton-proton
             collision data at s=8 TeV. A likelihood-driven scan of a
             five-dimensional effective model focusing on the
             gaugino-higgsino and Higgs sector of the phenomenological
             minimal supersymmetric Standard Model is performed. This
             scan uses data from direct dark matter detection
             experiments, the relic dark matter density and precision
             flavour physics results. Further constraints from the ATLAS
             Higgs mass measurement and SUSY searches at LEP are also
             applied. A subset of models selected from this scan are used
             to assess the impact of the selected ATLAS searches in this
             five-dimensional parameter space. These ATLAS searches
             substantially impact those models for which the mass
             m(χ˜10) of the lightest neutralino is less than 65 GeV,
             excluding 86% of such models. The searches have limited
             impact on models with larger m(χ˜10) due to either heavy
             electroweakinos or compressed mass spectra where the mass
             splittings between the produced particles and the lightest
             supersymmetric particle is small.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP09(2016)175},
   Key = {fds321098}
}

@article{fds308129,
   Author = {Antos, J and Babik, M and Benjamin, D and Cabrera, S and Chan, AW and Chen,
             YC and Coca, M and Cooper, B and Farrington, S and Genser, K and Hatakeyama, K and Hou, S and Hsieh, TL and Jayatilaka, B and Jun, SY and Kotwal, AV and Kraan, AC and Lysak, R and Mandrichenko, IV and Murat, P and Robson, A and Savard, P and Siket, M and Stelzer, B and Syu, J and Teng,
             PK and Timm, SC and Tomura, T and Vataga, E and Wolbers,
             SA},
   Title = {Data processing model for the CDF experiment},
   Journal = {IEEE Transactions on Nuclear Science},
   Volume = {53},
   Number = {5},
   Pages = {2897-2906},
   Publisher = {Institute of Electrical and Electronics Engineers
             (IEEE)},
   Year = {2006},
   Month = {October},
   url = {http://dx.doi.org/10.1109/TNS.2006.881908},
   Abstract = {The data processing model for the CDF experiment is
             described. Data processing reconstructs events from parallel
             data streams taken with different combinations of physics
             event triggers and further splits the events into datasets
             of specialised physics interests. The design of the
             processing control system makes strict requirements on
             bookkeeping records, which trace the status of data flies
             and event contents during processing and storage. The
             computing architecture was updated to meet the mass data
             flow of the Run II data collection, recently upgraded to a
             maximum rate of 40 MByte/sec. The data processing facility
             consists of a large cluster of Linux computers with data
             movement managed by the CDF data handling system to a
             multi-petaByte Enstore tape library. The latest processing
             cycle has achieved a stable speed of 35 MByte/sec (3
             TByte/day). It can be readily scaled by increasing CPU and
             data-handling capacity as required. © 2006
             IEEE.},
   Doi = {10.1109/TNS.2006.881908},
   Key = {fds308129}
}

@article{fds327864,
   Author = {Sen, S and Kotwal, A and Chekanov, S and Gray, L and Tran, NV and Yu,
             SS},
   Title = {Detectors for superboosted τ-leptons at future circular
             colliders},
   Journal = {Proceedings of Science},
   Volume = {Part F128556},
   Year = {2016},
   Month = {January},
   Abstract = {We study the detector performance of τ-lepton
             identification variables at very high energy proton
             colliders. We study hadronically-decaying τ-leptons with
             transverse momentum in the TeV range. Calorimeters are
             benchmarked in various configurations in order to understand
             the impact of granularity and resolution on boosted
             τ-lepton discrimination.},
   Key = {fds327864}
}

@article{fds354094,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Bourdarios, CA and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder,
             AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli,
             E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Pereira, RA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Determination of jet calibration and energy resolution in
             proton–proton collisions at √s=8TeV using the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {12},
   Year = {2020},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-08477-8},
   Abstract = {The jet energy scale, jet energy resolution, and their
             systematic uncertainties are measured for jets reconstructed
             with the ATLAS detector in 2012 using proton–proton data
             produced at a centre-of-mass energy of 8 TeV with an
             integrated luminosity of 20fb-1. Jets are reconstructed from
             clusters of energy depositions in the ATLAS calorimeters
             using the anti-kt algorithm. A jet calibration scheme is
             applied in multiple steps, each addressing specific effects
             including mitigation of contributions from additional
             proton–proton collisions, loss of energy in dead material,
             calorimeter non-compensation, angular biases and other
             global jet effects. The final calibration step uses several
             in situ techniques and corrects for residual effects not
             captured by the initial calibration. These analyses measure
             both the jet energy scale and resolution by exploiting the
             transverse momentum balance in γ + jet, Z + jet, dijet,
             and multijet events. A statistical combination of these
             measurements is performed. In the central detector region,
             the derived calibration has a precision better than 1% for
             jets with transverse momentum 150GeV<pT< 1500 GeV, and the
             relative energy resolution is (8.4 ± 0.6) % for pT=100GeV
             and (23 ± 2) % for pT=20GeV. The calibration scheme for
             jets with radius parameter R= 1.0 , for which jets receive a
             dedicated calibration of the jet mass, is also
             discussed.},
   Doi = {10.1140/epjc/s10052-020-08477-8},
   Key = {fds354094}
}

@article{fds310308,
   Author = {ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Piqueras, DÁ and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Beven, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
             S},
   Title = {Determination of spin and parity of the Higgs boson in the
             [Formula: see text] decay channel with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {5},
   Pages = {231},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3436-3},
   Abstract = {Studies of the spin and parity quantum numbers of the Higgs
             boson in the [Formula: see text] final state are presented,
             based on proton-proton collision data collected by the ATLAS
             detector at the Large Hadron Collider, corresponding to an
             integrated luminosity of 20.3 fb[Formula: see text] at a
             centre-of-mass energy of [Formula: see text] TeV. The
             Standard Model spin-parity [Formula: see text] hypothesis is
             compared with alternative hypotheses for both spin and CP.
             The case where the observed resonance is a mixture of the
             Standard-Model-like Higgs boson and CP-even ([Formula: see
             text]) or CP-odd ([Formula: see text]) Higgs boson in
             scenarios beyond the Standard Model is also studied. The
             data are found to be consistent with the Standard Model
             prediction and limits are placed on alternative spin and CP
             hypotheses, including CP mixing in different
             scenarios.},
   Doi = {10.1140/epjc/s10052-015-3436-3},
   Key = {fds310308}
}

@article{fds308226,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
             EW and Astur, R and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
             K and De, K and del Signore, K and Demarteau, M and Denisov, D and Denisov,
             SP and Diehl, HT and Diesburg, M and di Loreto, G and Draper, P and Ducros,
             Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvirai,
             VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
             OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feherg, S and Fein,
             D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum,
             E and Forden, GE},
   Title = {Determination of the absolute jet energy scale in the DO
             calorimeters},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {424},
   Number = {2},
   Pages = {352-394},
   Publisher = {Elsevier BV},
   Year = {1999},
   Month = {March},
   url = {http://dx.doi.org/10.1016/S0168-9002(98)01368-0},
   Abstract = {The DO detector is used to study pp collisions at the 1800
             and 630 GeV center-of-mass energies available at the
             Fermilab Tevatron. To measure jets, the detector uses a
             sampling calorimeter composed of uranium and liquid argon as
             the passive and active media, respectively, Understanding
             the jet energy calibration is not only crucial for precision
             tests of QCD, but also for the measurement of particle
             masses and the determination of physics backgrounds
             associated with new phenomena. This paper describes the
             energy calibration of jets observed with the DO detector at
             the two pp center-of-mass energies in the transverse energy
             and pseudorapidity range ET>8 GeV and |η|<3.},
   Doi = {10.1016/S0168-9002(98)01368-0},
   Key = {fds308226}
}

@article{fds308230,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
             V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Denisenko, N and Denisov, D and Denisov,
             SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
             Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak,
             Y},
   Title = {Determination of the mass of the W boson using the D
             detector at the Fermilab Tevatron},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {58},
   Number = {1},
   Pages = {120021+1200249},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.58.012002},
   Abstract = {A measurement of the mass of the [Formula Presented] boson
             is presented which is based on a sample of 5982 [Formula
             Presented] decays observed in [Formula Presented] collisions
             at [Formula Presented] TeV with the D detector during the
             1992–1993 run. From a fit to the transverse mass spectrum,
             combined with measurements of the [Formula Presented] boson
             mass, the [Formula Presented] boson mass is measured to be
             [Formula Presented] Detailed discussions of the
             determination of the absolute energy scale, the measured
             efficiencies, and all systematic uncertainties are
             presented. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.58.012002},
   Key = {fds308230}
}

@booklet{Abbott98e,
   Author = {B. Abbott and M. Abolins and B. S. Acharya and I. Adam and D. L. Adams and M. Adams and S. Ahn and H. Aihara and G. A.
             Alves and E. Amidi and N. Amos and E. W. Anderson and R.
             Astur and M. M. Baarmand and A. Baden and V. Balamurali and J. Balderston and B},
   Title = {Determination of the mass of the W boson using the D0
             detector at the Fermilab Tevatron},
   Journal = {Physical Review D},
   Volume = {5801},
   Number = {1},
   Year = {1998},
   Month = {July},
   Key = {Abbott98e}
}

@article{fds358462,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
             JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
             V and Arcangeletti, C and Arce, ATH and Arguin, JF and Argyropoulos,
             S},
   Title = {Determination of the parton distribution functions of the
             proton from ATLAS measurements of differential
             W± and Z boson production in association with
             jets},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {7},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2021)223},
   Abstract = {This article presents a new set of proton parton
             distribution functions, ATLASepWZVjet20, produced in an
             analysis at next-to-next-to-leading order in QCD. The new
             data sets considered are the measurements of W+ and W−
             boson and Z boson production in association with jets in pp
             collisions at s = 8 TeV performed by the ATLAS experiment at
             the LHC with integrated luminosities of 20.2 fb−1 and 19.9
             fb−1, respectively. The analysis also considers the ATLAS
             measurements of differential W± and Z boson production at s
             = 7 TeV with an integrated luminosity of 4.6 fb−1 and
             deep-inelastic-scattering data from e±p collisions at the
             HERA accelerator. An improved determination of the sea-quark
             densities at high Bjorken x is shown, while confirming a
             strange-quark density similar in size to the up- and
             down-sea-quark densities in the range x ≲ 0.02 found by
             previous ATLAS analyses. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP07(2021)223},
   Key = {fds358462}
}

@article{fds363730,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
             SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
             MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce,
             ATH},
   Title = {Determination of the parton distribution functions of the
             proton using diverse ATLAS data from pp collisions at √s=7
             , 8 and 13 TeV},
   Journal = {European Physical Journal C},
   Volume = {82},
   Number = {5},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2022},
   Month = {May},
   url = {http://dx.doi.org/10.1140/epjc/s10052-022-10217-z},
   Abstract = {This paper presents an analysis at next-to-next-to-leading
             order in the theory of quantum chromodynamics for the
             determination of a new set of proton parton distribution
             functions using diverse measurements in pp collisions at
             s=7, 8 and 13 TeV, performed by the ATLAS experiment at the
             Large Hadron Collider, together with deep inelastic
             scattering data from ep collisions at the HERA collider. The
             ATLAS data sets considered are differential cross-section
             measurements of inclusive W± and Z/ γ∗ boson production,
             W± and Z boson production in association with jets, tt¯
             production, inclusive jet production and direct photon
             production. In the analysis, particular attention is paid to
             the correlation of systematic uncertainties within and
             between the various ATLAS data sets and to the impact of
             model, theoretical and parameterisation uncertainties. The
             resulting set of parton distribution functions is called
             ATLASpdf21.},
   Doi = {10.1140/epjc/s10052-022-10217-z},
   Key = {fds363730}
}

@article{fds313614,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T},
   Title = {Determination of the Ratio of b-Quark Fragmentation
             Fractions f(s)/f(d) in pp Collisions at √s=7  TeV with
             the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {115},
   Number = {26},
   Pages = {262001},
   Year = {2015},
   Month = {December},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.115.262001},
   Abstract = {With an integrated luminosity of 2.47  fb(-1) recorded
             by the ATLAS experiment at the LHC, the exclusive decays
             B(s)(0)→J/ψϕ and B(d)(0)→J/ψK(*0) of B mesons
             produced in pp collisions at √s=7  TeV are used to
             determine the ratio of fragmentation fractions f(s)/f(d).
             From the observed B(s)(0)→J/ψϕ and B(d)(0)→J/ψK(*0)
             yields, the quantity (f(s)/f(d))[B(B(s)(0)→J/ψϕ)/B(B(d)(0)→J/ψK(*0))]
             is measured to be 0.199±0.004(stat)±0.008(syst). Using a
             recent theory prediction for [B(B(s)(0)→J/ψϕ)/B(B(d)(0)→J/ψK(*0))]
             yields (f(s)/f(d))=0.240±0.004(stat)±0.010(syst)±0.017(th).
             This result is based on a new approach that provides a
             significant improvement of the world average.},
   Doi = {10.1103/physrevlett.115.262001},
   Key = {fds313614}
}

@article{fds307693,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Determination of the strange-quark density of the proton
             from ATLAS measurements of the W→ℓν and Z→ℓℓ
             cross sections.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {1},
   Pages = {012001},
   Year = {2012},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.109.012001},
   Abstract = {A QCD analysis is reported of ATLAS data on inclusive W(±)
             and Z boson production in pp collisions at the LHC, jointly
             with ep deep-inelastic scattering data from HERA. The ATLAS
             data exhibit sensitivity to the light quark sea composition
             and magnitude at Bjorken x∼0.01. Specifically, the data
             support the hypothesis of a symmetric composition of the
             light quark sea at low x. The ratio of the strange-to-down
             sea quark distributions is determined to be
             1.00(-0.28)(+0.25) at absolute four-momentum transfer
             squared Q(2)=1.9  GeV(2) and x=0.023.},
   Doi = {10.1103/physrevlett.109.012001},
   Key = {fds307693}
}

@article{fds348506,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic,
             M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz,
             T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black,
             KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou,
             Y},
   Title = {Determination of the strong coupling constant α s from
             transverse energy-energy correlations in multijet events at
             s = 8 TeV using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {12},
   Pages = {872},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5442-0},
   Abstract = {Measurements of transverse energy-energy correlations and
             their associated asymmetries in multi-jet events using the
             ATLAS detector at the LHC are presented. The data used
             correspond to s = 8 TeV proton-proton collisions with an
             integrated luminosity of 20.2 fb - 1 . The results are
             presented in bins of the scalar sum of the transverse
             momenta of the two leading jets, unfolded to the particle
             level and compared to the predictions from Monte Carlo
             simulations. A comparison with next-to-leading-order
             perturbative QCD is also performed, showing excellent
             agreement within the uncertainties. From this comparison,
             the value of the strong coupling constant is extracted for
             different energy regimes, thus testing the running of α s (
             μ ) predicted in QCD up to scales over 1 TeV . A global fit
             to the transverse energy-energy correlation distributions
             yields α s ( m Z ) = 0.1162 ± 0.0011 (exp.) - 0.0070 +
             0.0084 (theo.) , while a global fit to the asymmetry
             distributions yields a value of α s ( m Z ) = 0.1196 ±
             0.0013 (exp.) - 0.0045 + 0.0075 (theo.) .},
   Doi = {10.1140/epjc/s10052-017-5442-0},
   Key = {fds348506}
}

@article{fds313610,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Determination of the top-quark pole mass using tt¯tt¯ +
             1-jet events collected with the ATLAS experiment in 7 TeV pp
             collisions},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2015)121},
   Abstract = {Abstract: The normalized differential cross section for
             top-quark pair production in association with at least one
             jet is studied as a function of the inverse of the invariant
             mass of the tt¯(Formula presented.) + 1-jet system. This
             distribution can be used for a precise determination of the
             top-quark mass since gluon radiation depends on the mass of
             the quarks. The experimental analysis is based on
             proton-proton collision data collected by the ATLAS detector
             at the LHC with a centre-of-mass energy of 7 TeV
             corresponding to an integrated luminosity of 4.6 fb−1. The
             selected events were identified using the lepton+jets
             top-quark-pair decay channel, where lepton refers to either
             an electron or a muon. The observed distribution is compared
             to a theoretical prediction at next-to-leading-order
             accuracy in quantum chromodynamics using the pole-mass
             scheme. With this method, the measured value of the
             top-quark pole mass, mtpole, is:mtpole=173.7±1.5stat.±1.4syst.−0.5+1.0theoryGeV.(Formula
             presented.). This result represents the most precise
             measurement of the top-quark pole mass to date.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP10(2015)121},
   Key = {fds313610}
}

@article{fds308263,
   Author = {Troutman, RR and Kotwal, A},
   Title = {Device model for the amorphous-silicon staggered-electrode
             thin-film transistor},
   Journal = {IEEE Transactions on Electron Devices},
   Volume = {36},
   Number = {12},
   Pages = {2915-2922},
   Year = {1989},
   url = {http://dx.doi.org/10.1109/16.40955},
   Abstract = {A model for the amorphous-silicon (a-Si) staggered-electrode
             thin-film transistor (TFT) that incorporates gate-voltage
             dependent mobility for channel current and
             space-charge-limited current effects for the source and
             drain contacts is discussed. This model is in excellent
             agreement with TFT data over a wide range of applied
             voltages and for various channel lengths. For the devices
             measured, the TFT current depends more sensitively on
             effective channel mobility than on space-charge-limited
             current through the a-Si layer, but the latter is
             responsible for current crowding at low drain voltage.
             Because of the two-dimensional current flow under the
             contacts, their equivalent lumped element model exhibits a
             different power law behavior than that for one-dimensional
             current flow in an n+-i-n+ structure. It also shows that a
             peak in the differential conductance curve at low drain
             voltage is a sensitive indicator of current crowding and
             implies a superlinear equivalent lumped element in series
             with the intrinsic TFT.},
   Doi = {10.1109/16.40955},
   Key = {fds308263}
}

@article{fds346173,
   Author = {Farid, M and Nicholson, S and Kotwal, A and Akali,
             A},
   Title = {DIEP breast reconstruction following multiple abdominal
             liposuction procedures.},
   Journal = {Eplasty},
   Volume = {14},
   Pages = {e47},
   Year = {2014},
   Month = {January},
   Abstract = {<h4>Objective</h4>Previous abdominal wall surgery is viewed
             as a contraindication to abdominal free tissue transfer. We
             present two patients who underwent multiple abdominal
             liposuction procedures, followed by successful free deep
             inferior epigastric artery perforator flap. We review the
             literature pertaining to reliability of abdominal free flaps
             in those with previous abdominal surgery.<h4>Methods</h4>Review
             of case notes and radiological investigations of two
             patients, and a PubMed search using the terms "DIEP", "deep
             inferior epigastric", "TRAM", "transverse rectus abdominis",
             "perforator" and "laparotomy", "abdominal wall",
             "liposuction", "liposculpture", "fat graft", "pfannenstiel",
             with subsequent appraisal of relevant papers by the first
             and second authors.<h4>Results</h4>Patient 1 had 3 episodes
             of liposuction from the abdomen for fat grafting to a
             reconstructed breast. Subsequent revision reconstruction of
             the same breast with DIEP flap was preceded by CT
             angiography, which demonstrated normal perforator anatomy.
             The reconstruction healed well with no ischaemic
             complications. Patient 2 had 5 liposuction procedures from
             the abdomen to graft fat to a wide local excision defect.
             Recurrence of cancer led to mastectomy and immediate
             reconstruction with free DIEP flap. Preoperative MR
             angiography demonstrated a large perforator right of the
             umbilicus, with which the intraoperative findings were
             consistent. The patient had an uneventful recovery and good
             healing with no fat necrosis or wound dehiscence.<h4>Conclusions</h4>We
             demonstrate that DIEP flaps can safely be raised without
             perfusion-related complications following multiple
             liposuction procedures to the abdomen. The safe interval
             between procedures is difficult to quantify, but we
             demonstrate successful free flap after 16
             months.},
   Key = {fds346173}
}

@article{fds308189,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev,
             VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett,
             JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings,
             MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del
             Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and di Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A},
   Title = {Differential cross section for w boson production as a
             function of transverse momentum in p p̄ collisions at √s
             = 1.8 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {513},
   Number = {3-4},
   Pages = {292-300},
   Publisher = {Elsevier BV},
   Year = {2001},
   Month = {August},
   url = {http://dx.doi.org/10.1016/S0370-2693(01)00628-1},
   Abstract = {We report a measurement of the differential cross section
             for W boson production as a function of its transverse
             momentum in proton-antiproton collisions at √s = 1.8 TeV.
             The data were collected by the DØ experiment at the
             Fermilab Tevatron Collider during 1994-1995 and correspond
             to an integrated luminosity of 85 pb-1. The results are in
             good agreement with quantum chromodynamics over the entire
             range of transverse momentum. © 2001 Elsevier Science
             B.V.},
   Doi = {10.1016/S0370-2693(01)00628-1},
   Key = {fds308189}
}

@article{fds355440,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MM and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R},
   Title = {Differential cross-section measurements for the electroweak
             production of dijets in association with a Z boson in
             proton–proton collisions at ATLAS},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {2},
   Year = {2021},
   Month = {February},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-08734-w},
   Abstract = {Differential cross-section measurements are presented for
             the electroweak production of two jets in association with a
             Z boson. These measurements are sensitive to the
             vector-boson fusion production mechanism and provide a
             fundamental test of the gauge structure of the Standard
             Model. The analysis is performed using proton–proton
             collision data collected by ATLAS at s=13TeV and with an
             integrated luminosity of 139fb-1. The differential
             cross-sections are measured in the Z→ ℓ+ℓ- decay
             channel (ℓ= e, μ) as a function of four observables: the
             dijet invariant mass, the rapidity interval spanned by the
             two jets, the signed azimuthal angle between the two jets,
             and the transverse momentum of the dilepton pair. The data
             are corrected for the effects of detector inefficiency and
             resolution and are sufficiently precise to distinguish
             between different state-of-the-art theoretical predictions
             calculated using Powheg+Pythia8, Herwig7+Vbfnlo and
             Sherpa 2.2. The differential cross-sections are used to
             search for anomalous weak-boson self-interactions using a
             dimension-six effective field theory. The measurement of the
             signed azimuthal angle between the two jets is found to be
             particularly sensitive to the interference between the
             Standard Model and dimension-six scattering amplitudes and
             provides a direct test of charge-conjugation and parity
             invariance in the weak-boson self-interactions.},
   Doi = {10.1140/epjc/s10052-020-08734-w},
   Key = {fds355440}
}

@article{fds308197,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
             M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and del
             Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
             HT and Diesburg, M and di Loreto, G and Draper, P and Ducros, Y and Dudko,
             LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
             VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
             OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T},
   Title = {Differential production cross section of Z bosons as a
             function of transverse momentum at √s = 1.8
             TeV},
   Journal = {Physical Review Letters},
   Volume = {84},
   Number = {13},
   Pages = {2792-2797},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevLett.84.2792},
   Abstract = {We present a measurement of the transverse momentum
             distribution of Z bosons produced in pp collisions at √s =
             1.8 TeV from data collected by the D experiment at the
             Fermilab Tevatron Collider. We find good agreement between
             our results and current resummation calculations, and also
             use our data to extract nonperturbative parameters for a
             particular version of the resummation formalism. The
             resulting values are significantly more precise than
             obtained in previous determinations. © 2000 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.84.2792},
   Key = {fds308197}
}

@article{fds321137,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
             M},
   Title = {Differential top-antitop cross-section measurements as a
             function of observables constructed from final-state
             particles using pp collisions at √s = 7 TeV in the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {6},
   Pages = {1-56},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2015)100},
   Abstract = {Abstract: Various differential cross-sections are measured
             in top-quark pair (tt) events produced in proton-proton
             collisions at a centre-of-mass energy of √s = 7 TeV at the
             LHC with the ATLAS detector. These differential
             cross-sections are presented in a data set corresponding to
             an integrated luminosity of 4.6 fb−1. The differential
             cross-sections are presented in terms of kinematic
             variables, such as momentum, rapidity and invariant mass, of
             a top-quark proxy referred to as the pseudo-top-quark as
             well as the pseudo-top-quark pair system. The dependence of
             the measurement on theoretical models is minimal. The
             measurements are performed on tt events in the lepton+jets
             channel, requiring exactly one charged lepton and at least
             four jets with at least two of them tagged as originating
             from a b-quark. The hadronic and leptonic pseudo-top-quarks
             are defined via the leptonic or hadronic decay mode of the W
             boson produced by the top-quark decay in events with a
             single charged lepton. Differential cross-section
             measurements of the pseudo-top-quark variables are compared
             with several Monte Carlo models that implement
             next-to-leading order or leading-order multi-leg
             matrix-element calculations.},
   Doi = {10.1007/JHEP06(2015)100},
   Key = {fds321137}
}

@article{fds307930,
   Author = {Aaltonen, and T, and others},
   Title = {Diffractive $W$ and $Z$ production at the Fermilab
             Tevatron},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {11},
   Pages = {112004},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.112004},
   Abstract = {We report on a measurement of the fraction of events with a
             W or Z boson which are produced diffractively in p̄p
             collisions at √s=1.96TeV, using data from 0.6fb⊃-1 of
             integrated luminosity collected with the CDFII detector
             equipped with a Roman-pot spectrometer that detects the p̄
             from p̄+p→p̄+[X+W/Z]. We find that (1.00±0.11)% of Ws
             and (0.88±0.22)% of Zs are produced diffractively in a
             region of antiproton or proton fractional momentum loss ξ
             of 0.03<ξ<0.10 and 4-momentum transferred squared t of
             -1<t<0(GeV/c)2, where we account for the events in which the
             proton scatters diffractively while the antiproton
             dissociates, p̄+p→[X+W/Z]+p, by doubling the measured
             proton dissociation fraction. We also report on searches for
             W and Z production in double Pomeron exchange,
             p+p̄→p+[X+W/Z]+p̄, and on exclusive Z production,
             p̄+p→p̄+Z+p. No signal is seen above background for
             these processes, and comparisons are made with expectations.
             © 2010 The American Physical Society.},
   Doi = {10.1103/PhysRevD.82.112004},
   Key = {fds307930}
}

@article{fds307800,
   Author = {Aaltonen, T and Albrow, M and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
             W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F},
   Title = {Diffractive dijet production in p̄p collisions at
             √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.032009},
   Abstract = {We report on a study of diffractive dijet production in p̄p
             collisions at √s=1.96TeV using the CDF II detector at the
             Fermilab Tevatron p̄p collider. A data sample from 310pb -1
             of integrated luminosity collected by triggering on a high
             transverse energy jet, ETjet, in coincidence with a recoil
             antiproton detected in a Roman pot spectrometer is used to
             measure the ratio of single-diffractive to inclusive-dijet
             event rates as a function of xp ̄ of the interacting parton
             in the antiproton, the Bjorken-x, xBjp̄, and a Q2(ETjet)2
             in the ranges 10 -3<xBjp̄<10 -1 and 102<Q2<104GeV2,
             respectively. Results are presented for the region of
             p̄-momentum-loss fraction 0.03<ξ p̄<0.09 and a
             four-momentum transfer squared t p̄>-4GeV2. The t p̄
             dependence is measured as a function of Q2 and xBjp̄ and
             compared with that of inclusive single diffraction
             dissociation. We find weak xBjp̄ and Q2 dependencies in the
             ratio of single diffractive to inclusive event rates, and no
             significant Q2 dependence in the diffractive t p̄
             distributions. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.86.032009},
   Key = {fds307800}
}

@booklet{Adams97a,
   Author = {M. R. Adams and M. Aderholz and S. Aid and P. L. Anthony and D. A. Averill and M. D. Baker and B. R. Baller and A.
             Banerjee and H. M. Braun and T. J. Carroll and H. L. Clark and J. M. Conrad and R. Davisson and I. Derado and A. A.
             Bhatti and U. Bratzler a},
   Title = {Diffractive production of rho(0)(770) mesons in muon-proton
             interactions at 470 GeV},
   Journal = {Zeitschrift Fur Physik C-particles And Fields},
   Volume = {74},
   Number = {2},
   Pages = {237 -- 261},
   Year = {1997},
   Month = {April},
   Key = {Adams97a}
}

@article{fds308251,
   Author = {Adams, MR and Aderholz, M and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dietrich, FS and Dougherty, W and Dreyer, T and Eckardt,
             V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen, KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Jackson, HE and Jaffe, DE and Jancso, G and Jansen, DM and Jin, Z and Kadija, K and Kaufmann, S and Kennedy, RD and Kinney, ER and Kobrak, HGE and Kotwal, AV and Kunori, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin,
             JG and Nickerson, RB and Novak, J and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou, V and Pawlik, B and Pipkin, FM and Potterveld, DH and Röser, A and Ryan, JJ and Salgado, CW and Schellman,
             H and Schmitt, M and Schmitz, N and Schüler, KP and Siegert, G and Skuja,
             A and Snow, GA and Söldner-Rembold, S and Spentzouris, P and Stopa, P and Swanson, RA and Venkataramania, H and Wilhelm, M and Wilson, R and Wittek, W and Wolbers, SA and Zeller, GP and Zghiche, A and Zhao,
             T},
   Title = {Diffractive production of ρ0(770) mesons in
             muon-proton interactions at 470 GeV},
   Journal = {Zeitschrift fur Physik C-Particles and Fields},
   Volume = {74},
   Number = {2},
   Pages = {237-261},
   Publisher = {Springer Nature},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1007/s002880050386},
   Abstract = {The diffractive production of ρ0(770) mesons in muon-proton
             interactions is studied in the kinematic region 0.15 GeV2 <
             Q2 < 20 GeV2 and 20 GeV < v < 420 GeV. The data were
             obtained in the Fermilab fixed-target experiment E665 with
             primary muons of 470 GeV energy. Results are presented on
             the Q2, x and v dependence of the cross section, on the
             shape of the π+π- mass spectrum, on the slope of the
             diffraction peak and on the production and decay angular
             distributions of the ρ0(770). The cross section for
             diffractive production of ρ0 by virtual photons on protons
             depends mainly on Q2. At fixed Q2, no significant dependence
             on x or v is observed. The extrapolation to Q2 = 0 yields a
             photoproduction cross section of (10.30 ± 0.33) μb. The
             slope of the t′ distribution has a value of (7.0 ± 0.2)
             GeV-2, with a tendency to decrease as Q2 increases. The
             production and decay angular distributions of the ρ0 depend
             strongly on Q2 and are consistent with s-channel helicity
             conservation. The ratio R = σL/σT deduced from the decay
             angular distributions rises strongly with Q2, passing the
             value of 1 at Q2 ≈ 2 GeV2. © Springer-Verlag
             1997.},
   Doi = {10.1007/s002880050386},
   Key = {fds308251}
}

@article{fds356577,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli,
             E and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini,
             MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Arduh, FA and Arguin,
             JF and Argyropoulos, S and Arling, JH and Armbruster,
             AJ},
   Title = {Dijet azimuthal correlations and conditional yields in pp
             and p+Pb collisions at sNN=5.02TeV with the ATLAS
             detector},
   Journal = {Physical Review C},
   Volume = {100},
   Number = {3},
   Year = {2019},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevC.100.034903},
   Abstract = {This paper presents a measurement of forward-forward and
             forward-central dijet azimuthal angular correlations and
             conditional yields in proton-proton (pp) and proton-lead
             (p+Pb) collisions as a probe of the nuclear gluon density in
             regions where the fraction of the average momentum per
             nucleon carried by the parton entering the hard scattering
             is low. In these regions, gluon saturation can modify the
             rapidly increasing parton distribution function of the
             gluon. The analysis utilizes 25pb-1 of pp data and 360μb-1
             of p+Pb data, both at sNN=5.02 TeV, collected in 2015 and
             2016, respectively, with the ATLAS detector at the Large
             Hadron Collider. The measurement is performed in the
             center-of-mass frame of the nucleon-nucleon system in the
             rapidity range between -4.0 and 4.0 using the two highest
             transverse-momentum jets in each event, with the highest
             transverse-momentum jet restricted to the forward rapidity
             range. No significant broadening of azimuthal angular
             correlations is observed for forward-forward or
             forward-central dijets in p+Pb compared to pp collisions.
             For forward-forward jet pairs in the proton-going direction,
             the ratio of conditional yields in p+Pb collisions to those
             in pp collisions is suppressed by approximately 20%, with no
             significant dependence on the transverse momentum of the
             dijet system. No modification of conditional yields is
             observed for forward-central dijets.},
   Doi = {10.1103/PhysRevC.100.034903},
   Key = {fds356577}
}

@article{fds308214,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Balamurali, V and Baldin, B and Banerjee,
             S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding,
             F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey,
             D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang,
             SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger,
             C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
             P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
             G},
   Title = {Dijet mass spectrum and a search for quark compositeness in
             (p)p collisions at sqrt(s) = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {82},
   Number = {12},
   Pages = {2457-2462},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.82.2457},
   Abstract = {Using the DZero detector at the 1.8 TeV pbarp Fermilab
             Tevatron collider, we have measured the inclusive dijet mass
             spectrum in the central pseudorapidity region |eta_jet| <
             1.0 for dijet masses greater than 200 Gev/c^2. We have also
             measured the ratio of spectra sigma(|eta_jet| <
             0.5)/sigma(0.5 < |eta_jet| < 1.0). The order alpha_s^3 QCD
             predictions are in good agreement with the data and we rule
             out models of quark compositeness with a contact interaction
             scale < 2.4 TeV at the 95% confidence level. © 1999 The
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.82.2457},
   Key = {fds308214}
}

@article{fds356774,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Dijet production in √s=7 TeV pp collisions with large
             rapidity gaps at the ATLAS experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {754},
   Pages = {214-234},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.01.028},
   Abstract = {A 6.8 nb−1 sample of pp collision data collected under
             low-luminosity conditions at s=7TeV by the ATLAS detector at
             the Large Hadron Collider is used to study diffractive dijet
             production. Events containing at least two jets with
             pT>20GeV are selected and analysed in terms of variables
             which discriminate between diffractive and non-diffractive
             processes. Cross sections are measured differentially in
             ΔηF, the size of the observable forward region of
             pseudorapidity which is devoid of hadronic activity, and in
             an estimator, ξ˜ of the fractional momentum loss of the
             proton assuming single diffractive dissociation (pp→pX).
             Model comparisons indicate a dominant non-diffractive
             contribution up to moderately large ΔηF and small ξ˜
             with a diffractive contribution which is significant at the
             highest ΔηF and the lowest ξ˜. The rapidity-gap survival
             probability is estimated from comparisons of the data in
             this latter region with predictions based on diffractive
             parton distribution functions.},
   Doi = {10.1016/j.physletb.2016.01.028},
   Key = {fds356774}
}

@article{fds352894,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asai,
             K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou,
             EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis,
             C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji,
             S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Besson,
             N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman,
             M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich,
             C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona,
             M and Bonilla, JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler,
             S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burr, JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba,
             LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carratta, G and Carter, JWS and Carter,
             TM and Casado, MP and Casha, AF and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
             DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen,
             J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng,
             HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chow, YS and Christopher, LD and Chu, MC and Chu, X},
   Title = {Dijet Resonance Search with Weak Supervision Using
             sqrt[s]=13  TeV pp Collisions in the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {125},
   Number = {13},
   Pages = {131801},
   Year = {2020},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevlett.125.131801},
   Abstract = {This Letter describes a search for narrowly resonant new
             physics using a machine-learning anomaly detection procedure
             that does not rely on signal simulations for developing the
             analysis selection. Weakly supervised learning is used to
             train classifiers directly on data to enhance potential
             signals. The targeted topology is dijet events and the
             features used for machine learning are the masses of the two
             jets. The resulting analysis is essentially a
             three-dimensional search A→BC, for m_{A}∼O(TeV),
             m_{B},m_{C}∼O(100  GeV) and B, C are reconstructed as
             large-radius jets, without paying a penalty associated with
             a large trials factor in the scan of the masses of the two
             jets. The full run 2 sqrt[s]=13  TeV pp collision
             dataset of 139  fb^{-1} recorded by the ATLAS detector
             at the Large Hadron Collider is used for the search. There
             is no significant evidence of a localized excess in the
             dijet invariant mass spectrum between 1.8 and 8.2 TeV.
             Cross-section limits for narrow-width A, B, and C particles
             vary with m_{A}, m_{B}, and m_{C}. For example, when
             m_{A}=3  TeV and m_{B}≳200  GeV, a production
             cross section between 1 and 5 fb is excluded at
             95% confidence level, depending on m_{C}. For certain
             masses, these limits are up to 10 times more sensitive than
             those obtained by the inclusive dijet search. These results
             are complementary to the dedicated searches for the case
             that B and C are standard model bosons.},
   Doi = {10.1103/physrevlett.125.131801},
   Key = {fds352894}
}

@article{fds307962,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar, P and Beecher, D and Behari, S and Bellettini,
             G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Copic, K and Cordelli, M and Cortiana, G and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
             S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni,
             GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest,
             R and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
             M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber,
             C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper,
             S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas,
             D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Koay, SA and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll,
             J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino,
             CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín,
             R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
             A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao,
             T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Movilla Fernandez and P and Mülmenstädt,
             J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura,
             K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert,
             B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi,
             F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers,
             E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber,
             I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer,
             B},
   Title = {Direct bound on the total decay width of the top quark in pp
             collisions at sqrt[s]=1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {4},
   Pages = {042001},
   Year = {2009},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.102.042001},
   Abstract = {We present the first direct experimental bound on the total
             decay width of the top quark, Gamma(t), using 955 pb(-1) of
             the Tevatron's pp collisions recorded by the Collider
             Detector at Fermilab. We identify 253 top-antitop pair
             candidate events. The distribution of reconstructed top
             quark mass from these events is fitted to templates
             representing different values of the top quark width. Using
             a confidence interval based on likelihood-ratio ordering, we
             extract an upper limit at 95% C.L. of Gamma(t)<13.1 GeV for
             an assumed top quark mass of 175 GeV/c(2).},
   Doi = {10.1103/physrevlett.102.042001},
   Key = {fds307962}
}

@article{fds365671,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
             SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
             MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei,
             D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH},
   Title = {Direct constraint on the Higgs–charm coupling from a
             search for Higgs boson decays into charm quarks with the
             ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {82},
   Number = {8},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2022},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-022-10588-3},
   Abstract = {A search for the Higgs boson decaying into a pair of charm
             quarks is presented. The analysis uses proton–proton
             collisions to target the production of a Higgs boson in
             association with a leptonically decaying W or Z boson. The
             dataset delivered by the LHC at a centre-of-mass energy of
             [InlineEquation not available: see fulltext.] and recorded
             by the ATLAS detector corresponds to an integrated
             luminosity of 139 fb-1. Flavour-tagging algorithms are used
             to identify jets originating from the hadronisation of charm
             quarks. The analysis method is validated with the
             simultaneous measurement of WW, WZ and ZZ production, with
             observed (expected) significances of 2.6 (2.2) standard
             deviations above the background-only prediction for the (W/
             Z) Z(→ cc¯) process and 3.8 (4.6) standard deviations for
             the (W/ Z) W(→ cq) process. The (W/ Z) H(→ cc¯) search
             yields an observed (expected) upper limit of 26 (31) times
             the predicted Standard Model cross-section times branching
             fraction for a Higgs boson with a mass of [InlineEquation
             not available: see fulltext.], corresponding to an observed
             (expected) constraint on the charm Yukawa coupling modifier
             |κc|<8.5(12.4), at the 95% confidence level. A combination
             with the ATLAS (W/ Z) H, H→ bb¯ analysis is performed,
             allowing the ratio κc/ κb to be constrained to less than
             4.5 at the 95% confidence level, smaller than the ratio of
             the b- and c-quark masses, and therefore determines the
             Higgs-charm coupling to be weaker than the Higgs-bottom
             coupling at the 95% confidence level.},
   Doi = {10.1140/epjc/s10052-022-10588-3},
   Key = {fds365671}
}

@booklet{Abachi97a,
   Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
             HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard, J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
             MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
             G},
   Title = {Direct measurement of the top quark mass},
   Journal = {Physical Review Letters},
   Volume = {79},
   Number = {7},
   Pages = {1197-1202},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.1197},
   Abstract = {We measure the top quark mass mt t¯t using pairs produced
             in the D0 detector by √s = 1.8 TeV p ¯p collisions in a
             125pb-1 exposure at the Fermilab Tevatron. We make a two
             constraint fit to mt in t¯t → b W+ ¯bW- final states
             with one W decaying to q¯q and the other to ev or μ v.
             Events are binned in fit mass versus a measure of
             probability for events to be signal rather than background.
             Likelihood fits to the data yield mt = 17.3 ± 5.6 (stat) ±
             6.2(syst) GeV/c2. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.79.1197},
   Key = {Abachi97a}
}

@article{fds308240,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
             EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis,
             E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram,
             I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Signore, KD and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Loreto, GD and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Geld, TL and Genik, RJ and Genser, K and Gerber, CE and Gibbard, B and Glenn, S and Gobbi, B and Goldschmidt, A and Gómez, B and Gómez, G and Goncharov,
             PI and Solís, JLG and Gordon, H and Goss, LT and Gounder, K and Goussiou,
             A and Graf, N and Grannis, PD and Green, DR and Greenlee, H and Grim, G and Grinstein, S and Grossman, N and Grudberg, P and Grünendahl, S and Guglielmo, G and Guida, JA and Guida, JM and Gupta, A and Gurzhiev, SN and Gutierrez, P and Gutnikov, YE and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hedin, D and Heinson, AP and Heintz, U and Hernández-Montoya, R and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hsieh, F and Ting, H and Tong, H and Huehn,
             T and Ito, AS and James, E and Jaques, J and Jerger, SA and Jesik, R and Jiang, JZY and Joffe-Minor, T and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Jun, SY and Jung, CK and Kahn, S and Kalbfleisch, G and Kang, JS and Karmanov, D and Karmgard, D and Kehoe, R and Kelly, ML and Kim, CL and Kim, SK and Klatchko, A and Klima,
             B and Klopfenstein, C and Klyukhin, VI and Kochetkov, VI and Kohli, JM and Koltick, D and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kourlas, J and Kozelov, AV and Kozlovski, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kunori, S and Lami, S and Lander, R and Landry, F and Landsberg, G and Lauer, B and Leflat, A and Li,
             H and Li, J and Li-Demarteau, QZ and Lima, JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Liu, YC and Lobkowicz, F and Loken, SC and Lökös, S and Lueking, L and Lyon, AL and Maciel, AKA and Madaras, RJ and Madden, R and Magaña-Mendoza, L and Manankov, V and Mani, S and Mao,
             HS and Markeloff, R and Marshall, T and Martin, MI and Mauritz, KM and May,
             B and Mayorov, AA and McCarthy, R and McDonald, J and McKibben, T and McKinley, J and McMahon, T and Melanson, HL and Merkin, M and Merritt,
             KW and Miettinen, H and Mincer, A and Mishra, CS and Mokhov, N and Mondal,
             NK and Montgomery, HE and Mooney, P and Motta, HD and Murphy, C and Nang,
             F and Narain, M and Narasimham, VS and Narayanan, A and Neal, HA and Negret, JP and Nemethy, P and Norman, D and Oesch, L and Oguri, V and Oliveira, E and Oltman, E and Oshima, N and Owen, D and Padley, P and Para,
             A and Park, YM and Partridge, R and Parua, N and Paterno, M and Pawlik, B and Perkins, J and Peters, M and Piegaia, R and Piekarz, H and Pischalnikov,
             Y and Podstavkov, VM and Pope, BG and Prosper, HB and Protopopescu, S and Qian, J and Quintas, PZ and Raja, R and Rajagopalan, S and Ramirez, O and Rasmussen, L and Reucroft, S and Rijssenbeek, M and Rockwell, T and Roco, M and Roe, NA and Rubinov, P and Ruchti, R and Rutherfoord, J and Sánchez-Hernández, A and Santoro, A and Sawyer, L and Schamberger,
             RD and Schellman, H and Sculli, J and Shabalina, E and Shaffer, C and Shankar, HC and Shivpuri, RK and Shupe, M and Singh, H and Singh, JB and Sirotenko, V and Smart, W and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sood, PM and Sosebee,
             M and Sotnikova, N and Souza, M and Spadafora, AL and Steinbrück, G and Stephens, RW and Stevenson, ML and Stewart, D and Stichelbaut, F and Stoianova, DA and Stoker, D and Strauss, M and Streets, K and Strovink,
             M and Sznajder, A and Tamburello, P and Tarazi, J and Tartaglia, M and Thomas, TLT and Thompson, J and Trippe, TG and Tuts, PM and Varelas, N and Varnes, EW and Vititoe, D and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, G and Warchol, J and Watts, G and Wayne, M and Weerts, H and White,
             A and White, JT and Wightman, JA and Willis, S and Wimpenny, SJ and Wirjawan, JVD and Womersley, J and Won, E and Wood, DR and Xu, H and Yamada, R and Yamin, P and Yang, J and Yasuda, T and Yepes, P and Yoshikawa, C and Youssef, S and Yu, J and Yu, Y and Zhu, ZH and Zieminska,
             D and Zieminski, A and Zverev, EG and Zylberstejn,
             A},
   Title = {Direct measurement of the top quark mass by the DO
             Collaboration},
   Journal = {Physical Review D},
   Volume = {58},
   Number = {5},
   Pages = {DUMMY5},
   Year = {1998},
   Abstract = {We determine the top quark mass mt using tt pairs produced
             in the DØ detector by √s=1.8TeV pp collisions in a 125
             pb-1 exposure at the Fermilab Tevatron. We make a two
             constraint fit to m1 in tt→bW+bW- final states with one W
             boson decaying to qq and the other to ev or μv. Likelihood
             fits to the data yield mt(l+jets)= 173.3±5.6 (stat) ±5.5
             (syst) GeV/c2. When this result is combined with an analysis
             of events in which both W bosons decay into leptons, we
             obtain mt= 172.1 ±5.2 (stat) ±4.9 (syst) GeV/c2. An
             alternate analysis, using three constraint fits to fixed top
             quark masses, gives mt(l+ jets) = 176.0 ±7.9 (stat)± 4.8
             (syst) GeV/c2, consistent with the above result. Studies of
             kinematic distributions of the top quark candidates are also
             presented. © 1998 The American Physical
             Society.},
   Key = {fds308240}
}

@article{fds308239,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
             EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis,
             E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram,
             I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and del Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {Direct measurement of the top quark mass by the DØ
             Collaboration},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {58},
   Number = {5},
   Pages = {520011-520012+5200139},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {September},
   ISSN = {0556-2821},
   url = {http://dx.doi.org/10.1103/PhysRevD.58.052001},
   Abstract = {We determine the top quark mass mt using tt̄ pairs produced
             in the DØ deteetor by √s = 1.8 TeV pp̄ collisions in a
             125 ph-1 exposure at the Fermilab Tevatron. We make a two
             constraint fit to mt in tt̄→bW+b̄W- final states with
             one W boson decaying to qq̄ and the other to eν or μν.
             Likelihood fits to the data yield mt(l+jets) = 173.3±5.6
             (stat) ± 5.5 (syst) GeV/c2. When this result is combined
             with an analysis of events in which both W bosons decay into
             leptons, we obtain mt = 172.1 ± 5.2 (stat) ± 4.9 (syst)
             GeV/c2. An alternate analysis, using three constraint fits
             to fixed top quark masses, gives mt(l + jets) = 176.0 ± 7.9
             (stat) ± 4.8 (syst) GeV/c2, consistent with the above
             result. Studies of kinematic distributions of the top quark
             candidates are also presented.},
   Doi = {10.1103/PhysRevD.58.052001},
   Key = {fds308239}
}

@article{fds307566,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
             JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
             A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
             C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
             L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Direct measurement of the total decay width of the top
             quark.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {20},
   Pages = {202001},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.111.202001},
   Abstract = {We present a measurement of the total decay width of the top
             quark using events with top-antitop quark pair candidates
             reconstructed in the final state with one charged lepton and
             four or more hadronic jets. We use the full Tevatron run II
             data set of sqrt[s]=1.96  TeV proton-antiproton
             collisions recorded by the CDF II detector. The top quark
             mass and the mass of the hadronically decaying W boson are
             reconstructed for each event and compared with distributions
             derived from simulated signal and background samples to
             extract the top quark width (Γtop) and the energy scale of
             the calorimeter jets with in situ calibration. For a top
             quark mass Mtop=172.5  GeV/c2, we find
             1.10<Γtop<4.05  GeV at 68% confidence level, which is
             in agreement with the standard model expectation of 1.3 GeV
             and is the most precise direct measurement of the top quark
             width to date.},
   Doi = {10.1103/physrevlett.111.202001},
   Key = {fds307566}
}

@article{fds307953,
   Author = {Aaltonen, T and others},
   Title = {Direct Measurement of the W Production Charge Asymmetry in
             pp̅ Collisions at sqrt[s] =1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {18},
   Pages = {181801},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.181801},
   Abstract = {We present the first direct measurement of the W production
             charge asymmetry as a function of the W boson rapidity yW in
             pp̅ collisions at sqrt[s]=1.96  TeV. We use a sample of
             W→eν events in data from 1  fb-1 of integrated
             luminosity collected using the CDF II detector. In the
             region |yW|&lt;3.0, this measurement is capable of
             constraining the ratio of up- and down-quark momentum
             distributions in the proton more directly than in previous
             measurements of the asymmetry that are functions of the
             charged-lepton pseudorapidity.},
   Doi = {10.1103/physrevlett.102.181801},
   Key = {fds307953}
}

@article{fds308176,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev,
             VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett,
             JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings,
             MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del
             Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
             T and Feher, S and Fein, D and Ferbel, T and Filthaut, F and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin,
             R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grünendahl, S and Gupta,
             A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hildreth, MD and Hirosky,
             R and Hobbs, JD and Hoeneisen, B and Huang, Y and Illingworth, R and Ito,
             AS and Jaffré, M and Jain, S and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Kalinin, AM and Karmanov, D and Karmgard, D and Kehoe, R and Kharchilava, A and Kim, SK and Klima, B and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov,
             AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krivkova, P and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kuznetsov, VE and Landsberg, G and Leflat, A and Leggett, C and Lehner, F and Li, J and Li, QZ and Lima, JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AKA and Madaras, RJ and Malyshev,
             VL and Manankov, V and Mao, HS and Marshall, T and Martin, MI and Martin,
             RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy, R and McDonald,
             J and McMahon, T and Melanson, HL and Merkin, M and Merritt, KW and Miao,
             C and Miettinen, H and Mihalcea, D and Mishra, CS and Mokhov, N and Mondal,
             NK and Montgomery, HE and Moore, RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Nunnemann, T and O'Neil, D and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou, K and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Pétroff, P and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Qian, J and Raja, R and Rajagopalan,
             S and Ramberg, E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Sabirov, BM and Santoro, A and Sawyer,
             L and Schamberger, RD and Schellman, H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell,
             RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery,
             P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Strovink, M and Stutte, L and Sznajder,
             A and Taylor, W and Tentindo-Repond, S and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and van Gemmeren, P and Vaniev, V and Van
             Kooten, R and Varelas, N and Vertogradov, LS and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, Z-M and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Womersley, J and Wood, DR and Yamada, R and Yamin, P and Yasuda, T and Yatsunenko, YA and Yip, K and Youssef, S and Yu, J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev, EG and Zylberstejn, A and D0
             Collaboration},
   Title = {Direct search for charged higgs bosons in decays of top
             quarks.},
   Journal = {Physical review letters},
   Volume = {88},
   Number = {15},
   Pages = {151803},
   Year = {2002},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.88.151803},
   Abstract = {We present a search for charged Higgs bosons in decays of
             pair-produced top quarks in pp collisions at sqrt[s] = 1.8
             TeV recorded by the D0 detector at the Fermilab Tevatron
             collider. With no evidence for signal, we exclude most
             regions of the ( M(H+/-),tan(beta)) parameter space where
             the decay t--> H(+)b has a branching fraction >0.36 and
             B(H+/--->tau(nu)(tau)) is large.},
   Doi = {10.1103/physrevlett.88.151803},
   Key = {fds308176}
}

@article{fds308094,
   Author = {Abulencia, and A, and others},
   Title = {Direct search for Dirac magnetic monopoles in $p\bar{p}$
             collisions at $\sqrt{s} = 1.96$ TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {20},
   Pages = {201801},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.201801},
   Abstract = {We search for pair-produced Dirac magnetic monopoles in 35.7
             pb-1 of proton-antiproton collisions at s**(1/2) = 1.96 TeV
             with the Collider Detector at Fermilab (CDF). We find no
             monopole candidates corresponding to a 95\% confidence-level
             cross-section limit sigma 360 GeV/c2.},
   Doi = {10.1103/physrevlett.96.201801},
   Key = {fds308094}
}

@article{fds347467,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Verzini, MJA and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos,
             SPA and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Ferraz,
             VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic,
             M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
             C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
             AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertram, IA and Bertsche, C and Besjes, GJ and Bylund,
             OB and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
             Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cai, H and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Bret,
             MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini,
             M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
             I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney,
             RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casper, DW and Castelijn, R and Gimenez,
             VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan,
             SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Direct top-quark decay width measurement in the t t ¯
             lepton+jets channel at s = 8 TeV with the ATLAS
             experiment.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {2},
   Pages = {129},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-5595-5},
   Abstract = {This paper presents a direct measurement of the decay width
             of the top quark using t t ¯ events in the lepton+jets
             final state. The data sample was collected by the ATLAS
             detector at the LHC in proton-proton collisions at a
             centre-of-mass energy of 8 TeV and corresponds to an
             integrated luminosity of 20.2 fb - 1 . The decay width of
             the top quark is measured using a template fit to
             distributions of kinematic observables associated with the
             hadronically and semileptonically decaying top quarks. The
             result, Γ t = 1.76 ± 0.33 ( stat. ) - 0.68 + 0.79 ( syst.
             ) GeV for a top-quark mass of 172.5 GeV, is consistent with
             the prediction of the Standard Model.},
   Doi = {10.1140/epjc/s10052-018-5595-5},
   Key = {fds347467}
}

@article{fds307895,
   Author = {Aaltonen, and T, and others},
   Title = {Direct Top-Quark Width Measurement at CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {23},
   Pages = {232003},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.232003},
   Abstract = {We present a measurement of the top-quark width in the
             lepton+jets decay channel of tt events produced in p p
             collisions at Fermilab's Tevatron collider and collected by
             the CDF II detector. From a data sample corresponding to 4.3
             fb(-1) of integrated luminosity, we identify 756 candidate
             events. The top-quark mass and the mass of the hadronically
             decaying W boson that comes from the top-quark decay are
             reconstructed for each event and compared with templates of
             different top-quark widths (Γ(t)) and deviations from
             nominal jet energy scale (Δ(JES)) to perform a simultaneous
             fit for both parameters, where Δ(JES) is used for the in
             situ calibration of the jet energy scale. By applying a
             Feldman-Cousins approach, we establish an upper limit at 95%
             confidence level (CL) of Γ(t) <7.6 GeV and a two-sided 68%
             CL interval of 0.3 GeV <Γ(t) <4.4  GeV for a top-quark
             mass of 172.5 GeV/c(2), which are consistent with the
             standard model prediction.},
   Doi = {10.1103/PhysRevLett.105.232003},
   Key = {fds307895}
}

@article{fds362580,
   Author = {Kotwal, AV and Hofmann, S},
   Title = {Discrete energy spectrum of Hawking radiation from
             Schwarzschild surfaces},
   Year = {2002},
   Month = {April},
   Abstract = {We analyze the allowed energy levels of Hawking radiation
             from Schwarzschild surfaces in space-times with large extra
             dimensions. From the requirement that the wave functions
             associated with these particles be single-valued and obey
             radial boundary conditions, we derive an upper bound of
             their discrete energy spectrum as a function of the number
             of large extra dimensions and the mass of the black hole.
             Furthermore, we investigate the spacing of the energy
             levels.},
   Key = {fds362580}
}

@article{fds347525,
   Author = {Kotwal, A and Kotwal, J and Prakash, R and Kotwal,
             N},
   Title = {Does iodine excess lead to hypothyroidism? Evidence from a
             case-control study in India.},
   Journal = {Archives of medical research},
   Volume = {46},
   Number = {6},
   Pages = {490-494},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.arcmed.2015.07.005},
   Abstract = {<h4>Background</h4>Iodine deficiency disorders have been
             known to mankind since antiquity and various researchers
             elucidated the role of iodine in its causation. However,
             recent evidence shows that the entire control program
             ignored multi-causality and association of increased iodine
             intake with hypothyroidism. This study was conducted to
             assess differences of iodine intake as measured by urinary
             iodine excretion (UIE) between cases of hypothyroidism and
             healthy controls.<h4>Methods</h4>A case-control study was
             conducted with three groups (cases, hospital controls and
             community controls) in two cities of India. Patients with
             overt hypothyroidism were cases (n = 150) and were
             compared with age, sex and socioeconomic status-matched
             hospital (n = 154) and community (n = 488) controls.
             Thyroid function tests (T3, T4, TSH) were used as diagnostic
             and inclusion criteria. TPOAb and UIE estimation were
             carried out for all study participants.<h4>Results</h4>Mean
             values of TPOAb and UIE were higher in cases as compared to
             hospital controls as well as community controls (p <0.05).
             With a cut off of 34 IU/mL for TPOAb, more cases had an
             anti-TPO level >34 as compared to hospital controls
             (p <0.001) as well as community controls (p <0.001); OR,
             0.06 (95% CI, 0.03, 0.12) and 0.08 (0.05, 0.12),
             respectively. For UIE cut-off of 300 μg/L, more cases than
             hospital controls (p = 0.090) and community controls
             (p = 0.001) had higher levels; OR, 0.671, (0.422, 1.066)
             and 0.509, (0.348, 0.744), respectively.<h4>Conclusion</h4>The
             study has clearly shown that cases of hypothyroidism are
             associated with excess iodine intake. Cohort studies to
             generate further evidence and an eco-social epidemiological
             approach have been suggested as the way forward.},
   Doi = {10.1016/j.arcmed.2015.07.005},
   Key = {fds347525}
}

@article{fds227089,
   Author = {A.V. Kotwal and S. Chekanov and M. Low},
   Title = {Double Higgs Boson Production in the 4tau Channel from
             Resonances in Longitudinal Vector Boson Scattering at a 100
             TeV Collider},
   Journal = {Phys.Rev. D.},
   Volume = {91},
   Number = {114018},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.114018},
   Doi = {10.1103/PhysRevD.91.114018},
   Key = {fds227089}
}

@article{fds310283,
   Author = {Kotwal, AV and Chekanov, S and Low, M},
   Title = {Double Higgs boson production in the 4τ channel from
             resonances in longitudinal vector boson scattering at a 100
             TeV collider},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.114018},
   Abstract = {We discuss the sensitivity of a 100 TeV pp collider to heavy
             resonances produced in longitudinal vector-boson scattering
             and decaying to a pair of Higgs bosons. A Monte Carlo study
             has been performed using the H→ττ decay channel for both
             Higgs bosons, comparing the kinematics of such a signal to
             the irreducible Standard Model backgrounds. The results are
             presented in the context of a phenomenological model of a
             resonance (η) coupling to Goldstone modes, VLVL→η→HH,
             as can arise in composite Higgs models. With a fractional
             width of 70% (20%), the 5σ discovery reach is 4.2 (2.9) TeV
             in resonance mass for 10ab-1 of integrated luminosity. We
             also discuss the dependence of the mass reach on the
             collider energy and integrated luminosity.},
   Doi = {10.1103/PhysRevD.91.114018},
   Key = {fds310283}
}

@article{fds307529,
   Author = {Kotwal, AV and Hays, CP},
   Title = {Drift chamber alignment using cosmic rays},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {762},
   Pages = {85-99},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.nima.2014.05.050},
   Abstract = {The Collider Detector at Fermilab (CDF) is a general-purpose
             experimental apparatus with an inner tracking detector for
             measuring charged particles, surrounded by a calorimeter for
             measurements of electromagnetic and hadronic showers and a
             muon detector system. We present a technique for, and
             results of, a precise relative alignment of the drift
             chamber wires of the CDF tracker. This alignment has been an
             important component of the track momentum calibration, which
             is the basis for the charged-lepton calibration for the
             measurement of the W boson mass at CDF. © 2014 Elsevier
             B.V.},
   Doi = {10.1016/j.nima.2014.05.050},
   Key = {fds307529}
}

@article{fds307646,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov,
             VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson,
             M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
             G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach,
             AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes,
             JB and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey,
             DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
             DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Costa, JBGD and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
             N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
             M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, JB and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Brown, G and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley,
             AG and Buda, SI and Budagov, IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Armadans,
             RC and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung,
             SL and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow,
             BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu,
             ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca,
             D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron,
             ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
             RN and Clemens, JC},
   Title = {Dynamics of isolated-photon plus jet production in pp
             collisions at s=7 TeV with the ATLAS detector},
   Journal = {Nuclear Physics B},
   Volume = {875},
   Number = {3},
   Pages = {483-535},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.nuclphysb.2013.07.025},
   Abstract = {The dynamics of isolated-photon plus jet production in pp
             collisions at a centre-of-mass energy of 7 TeV has been
             studied with the ATLAS detector at the LHC using an
             integrated luminosity of 37 pb-1. Measurements of
             isolated-photon plus jet bin-averaged cross sections are
             presented as functions of photon transverse energy, jet
             transverse momentum and jet rapidity. In addition, the
             bin-averaged cross sections as functions of the difference
             between the azimuthal angles of the photon and the jet, the
             photon-jet invariant mass and the scattering angle in the
             photon-jet centre-of-mass frame have been measured.
             Next-to-leading-order QCD calculations are compared to the
             measurements and provide a good description of the data,
             except for the case of the azimuthal opening angle. © 2013
             CERN.},
   Doi = {10.1016/j.nuclphysb.2013.07.025},
   Key = {fds307646}
}

@article{fds347523,
   Author = {Kotwal, J and Kotwal, A and Bhalla, S and Singh, PK and Nair,
             V},
   Title = {Effectiveness of homocysteine lowering vitamins in
             prevention of thrombotic tendency at high altitude area: A
             randomized field trial.},
   Journal = {Thrombosis research},
   Volume = {136},
   Number = {4},
   Pages = {758-762},
   Year = {2015},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.thromres.2015.08.001},
   Abstract = {<h4>Introduction</h4>A higher risk of thrombosis has been
             reported on prolonged stay at high altitude (HAA). Lowering
             of homocysteine (Hcy) has been found to reduce the risk of
             venous thrombosis. A randomized field trial was conducted
             with primary question whether Hcy lowering agents have any
             effect on the incidence of thrombosis at HAA amongst Indian
             soldiers as compared to existing interventions.<h4>Methods</h4>All
             units freshly inducted to HAA were randomized into
             intervention (Vit B12 1000 microgram/day, B6 3mg/day & folic
             acid 5mg/day) and control arms, with a sample size of 12,000
             person-years in each arm.<h4>Results</h4>At the end of one
             year stay at HAA, Folate and B 12 levels decreased
             significantly in control arm. The levels of Hcy, fibrinogen
             and plasminogen activator inhibitor (PAI 1) were lower and
             nitric oxide higher in intervention arm as compared to
             control arm (p<0.05). At the end of 2years, 5 thrombotic
             episodes occurred in the intervention arm and 17 in control
             arm with RR of 0.29 (95% CI 0.11-0.80), attributable
             fraction % (AFe) 70.59%, Population attributable risk
             percent 54.55% and Protective Fraction 240%.<h4>Conclusion</h4>Intervention
             with B12 and folic acid is effective in reducing Hcy, PAI 1,
             fibrinogen levels and increasing NO levels at 1yr as
             compared to control arm and reducing the incidence of
             thrombosis at 2years of stay at HAA. Thus, vitamin B 12, B6
             and folic acid intervention is safe and effective method of
             reducing morbidity and mortality caused by HAA induced
             coagulopathy.},
   Doi = {10.1016/j.thromres.2015.08.001},
   Key = {fds347523}
}

@article{fds347540,
   Author = {Kotwal, A and Biswas, D and Kakati, B and Thakuria, B and Bhardwaj,
             N},
   Title = {Efficacy of anti-pseudomonal antibiotics: need to reconsider
             the empirical use of cefepime.},
   Journal = {The Indian journal of medical research},
   Volume = {140},
   Number = {4},
   Pages = {560-562},
   Year = {2014},
   Month = {October},
   Key = {fds347540}
}

@article{fds346198,
   Author = {Londhe, SM and Kumar, P and Mitra, R and Kotwal, A},
   Title = {Efficacy of Second Molar to Achieve Anchorage Control in
             Maximum Anchorage Cases.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {66},
   Number = {3},
   Pages = {220-224},
   Year = {2010},
   Month = {July},
   url = {http://dx.doi.org/10.1016/s0377-1237(10)80041-3},
   Abstract = {<h4>Background</h4>The aim of the study was to assess the
             efficacy of inclusion of second molar in treatment at the
             outset to reinforce anchorage.<h4>Methods</h4>A comparative
             study comprising of 30 maximum anchorage cases to quantify
             anchorage loss in two situations was undertaken. Group I
             consisted of cases in which only first molars were banded
             and Group II consisted of cases where both first and second
             molars were banded. A total of seven landmarks were marked
             and six measurements were recorded on to the pre-treatment
             and post-treatment lateral cephalogram.<h4>Result</h4>The
             difference in pre-treatment and post-treatment values of all
             the variables were statistically significant (p<0.05) except
             maxillary central incisor vertical movement (U1 VER),
             implying a significant post-treatment change. Thus in both
             the treatment approaches U6 and U1 showed a considerable
             amount of movement in horizontal and vertical direction and
             there was rotation which brought about change in angular
             values.<h4>Conclusion</h4>The study has successfully
             quantified the anchorage loss and brought out the advantages
             of including second molar in treatment at the outset. Not
             only the anchorage loss is minimized but inclusion of second
             molar also helps to maximize incisor retraction and helps
             control angular movement of molar and incisor. Extra time
             required for second molar banding is well spent, as the
             benefits are overwhelming.},
   Doi = {10.1016/s0377-1237(10)80041-3},
   Key = {fds346198}
}

@article{fds346219,
   Author = {Kotwal, A and Schmidt, CE},
   Title = {Electrical stimulation alters protein adsorption and nerve
             cell interactions with electrically conducting
             biomaterials.},
   Journal = {Biomaterials},
   Volume = {22},
   Number = {10},
   Pages = {1055-1064},
   Year = {2001},
   Month = {May},
   url = {http://dx.doi.org/10.1016/s0142-9612(00)00344-6},
   Abstract = {Electrical charges have been shown to enhance nerve
             regeneration; however, the mechanisms for this effect are
             unclear. One hypothesis is that an electrical stimulus
             alters the local electrical fields of extracellular matrix
             molecules, changing protein adsorption. We have investigated
             this hypothesis--that electrical stimulation increases the
             adsorption of serum proteins, specifically fibronectin (FN),
             to the electrically conducting polymer polypyrrole (PP),
             thereby, increasing neurite extension. PP was used because
             electrical stimulation of PP has been shown to significantly
             enhance neurite outgrowth, and more importantly, PP can be
             formed into conduits to guide nerve regeneration in vivo.
             Here, we looked at the effects of electrical stimulation on
             protein adsorption when an electrical current was applied to
             PP (1) during protein adsorption (immediate stimulation) and
             (2) several hours after protein adsorption (delayed
             stimulation). We found that immediate stimulation of PP
             increases FN adsorption from purified FN and
             serum-containing solutions. Correspondingly, PC-12 cells
             grown on PP films that had been previously adsorbed with FN
             during immediate stimulation expressed longer neurites.
             However, for delayed stimulation, no significant differences
             in adsorption or neurite outgrowth were observed. These
             studies suggest that increased FN adsorption with immediate
             electrical stimulation may explain enhanced neurite
             extension on electrically stimulated PP.},
   Doi = {10.1016/s0142-9612(00)00344-6},
   Key = {fds346219}
}

@article{fds218204,
   Author = {A.V. Kotwal and C. Hays},
   Title = {Electromagnetic Shower Properties in a Lead-Scintillator
             Sampling Calorimeter},
   Journal = {Nuclear Inst. and Methods in Physics Research,
             A},
   Volume = {729},
   Pages = {25-35},
   Year = {2013},
   Month = {November},
   Key = {fds218204}
}

@article{fds307585,
   Author = {Kotwal, AV and Hays, C},
   Title = {Electromagnetic shower properties in a lead-scintillator
             sampling calorimeter},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {729},
   Pages = {25-35},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {July},
   url = {http://dx.doi.org/10.1016/j.nima.2013.05.185},
   Abstract = {The Collider Detector at Fermilab (CDF) is a general-purpose
             experimental apparatus with an inner tracking detector for
             measuring charged particles, surrounded by a calorimeter for
             measurements of electromagnetic and hadronic showers. We
             describe a geant4 simulation and parameterization of the
             response of the CDF central electromagnetic calorimeter
             (CEM) to incident electrons and photons. The detector model
             consists of a detailed description of the CEM geometry and
             material in the direction of the incident particle's
             trajectory, and of the passive material between the tracker
             and the CEM. We use geant4 to calculate the distributions
             of: the energy that leaks from the back of the CEM, the
             energy fraction sampled by the scintillators, and the energy
             dependence of the response. We parameterize these
             distributions to accurately model electron and photon
             response and resolution in a custom simulation for the
             measurement of the W boson mass. © 2013 Elsevier
             B.V.},
   Doi = {10.1016/j.nima.2013.05.185},
   Key = {fds307585}
}

@article{fds356616,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA},
   Title = {Electron and photon energy calibration with the ATLAS
             detector using 2015-2016 LHC proton-proton collision
             data},
   Journal = {Journal of Instrumentation},
   Volume = {14},
   Number = {3},
   Year = {2019},
   Month = {March},
   url = {http://dx.doi.org/10.1088/1748-0221/14/03/P03017},
   Abstract = {This paper presents the electron and photon energy
             calibration obtained with the ATLAS detector using about 36
             fb-1 of LHC proton-proton collision data recorded at s=13
             TeV in 2015 and 2016. The different calibration steps
             applied to the data and the optimization of the
             reconstruction of electron and photon energies are
             discussed. The absolute energy scale is set using a large
             sample of Z boson decays into electron-positron pairs. The
             systematic uncertainty in the energy scale calibration
             varies between 0.03% to 0.2% in most of the detector
             acceptance for electrons with transverse momentum close to
             45 GeV . For electrons with transverse momentum of 10 GeV
             the typical uncertainty is 0.3% to 0.8% and it varies
             between 0.25% and 1% for photons with transverse momentum
             around 60 GeV . Validations of the energy calibration with
             J/ψ → e+e- decays and radiative Z boson decays are also
             presented.},
   Doi = {10.1088/1748-0221/14/03/P03017},
   Key = {fds356616}
}

@article{fds310357,
   Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Electron and photon energy calibration with the ATLAS
             detector using LHC Run 1 data},
   Journal = {European Physical Journal C},
   Volume = {74},
   Number = {10},
   Pages = {1-48},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3071-4},
   Abstract = {This paper presents the electron and photon energy
             calibration achieved with the ATLAS detector using about
             25 fb-1 of LHC proton–proton collision data taken at
             centre-of-mass energies of (Equation Present) and 8 TeV.
             The reconstruction of electron and photon energies is
             optimised using multivariate algorithms. The response of the
             calorimeter layers is equalised in data and simulation, and
             the longitudinal profile of the electromagnetic showers is
             exploited to estimate the passive material in front of the
             calorimeter and reoptimise the detector simulation. After
             all corrections, the Z resonance is used to set the absolute
             energy scale. For electrons from Z decays, the achieved
             calibration is typically accurate to 0.05 % in most of the
             detector acceptance, rising to 0.2 % in regions with large
             amounts of passive material. The remaining inaccuracy is
             less than 0.2–1 % for electrons with a transverse energy
             of 10 GeV, and is on average 0.3 % for photons. The
             detector resolution is determined with a relative inaccuracy
             of less than 10 % for electrons and photons up to 60 GeV
             transverse energy, rising to 40 % for transverse energies
             above 500 GeV.},
   Doi = {10.1140/epjc/s10052-014-3071-4},
   Key = {fds310357}
}

@article{fds356553,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Achary, BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
             Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V},
   Title = {Electron and photon performance measurements with the ATLAS
             detector using the 2015-2017 LHC proton-proton collision
             data},
   Journal = {Journal of Instrumentation},
   Volume = {14},
   Number = {12},
   Year = {2019},
   Month = {December},
   url = {http://dx.doi.org/10.1088/1748-0221/14/12/P12006},
   Abstract = {This paper describes the reconstruction of electrons and
             photons with the ATLAS detector, employed for measurements
             and searches exploiting the complete LHC Run 2 dataset. An
             improved energy clustering algorithm is introduced, and its
             implications for the measurement and identification of
             prompt electrons and photons are discussed in detail.
             Corrections and calibrations that affect performance,
             including energy calibration, identification and isolation
             efficiencies, and the measurement of the charge of
             reconstructed electron candidates are determined using up to
             81 fb-1 of proton-proton collision data collected at √s =
             13 TeV between 2015 and 2017.},
   Doi = {10.1088/1748-0221/14/12/P12006},
   Key = {fds356553}
}

@article{fds347495,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
             H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten,
             K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
             A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and da
             Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev,
             A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
             Kuutmann, E and Berger, N and Beringer, J and Berlendis, S and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
             MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher,
             V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
             S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda,
             E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro,
             NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez
             Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
             S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El Moursli and RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
   Title = {Electron efficiency measurements with the ATLAS detector
             using 2012 LHC proton-proton collision data.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {3},
   Pages = {195},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4756-2},
   Abstract = {This paper describes the algorithms for the reconstruction
             and identification of electrons in the central region of the
             ATLAS detector at the Large Hadron Collider (LHC). These
             algorithms were used for all ATLAS results with electrons in
             the final state that are based on the 2012 <i>pp</i>
             collision data produced by the LHC at [Formula: see text] =
             8 [Formula: see text]. The efficiency of these algorithms,
             together with the charge misidentification rate, is measured
             in data and evaluated in simulated samples using electrons
             from [Formula: see text], [Formula: see text] and [Formula:
             see text] decays. For these efficiency measurements, the
             full recorded data set, corresponding to an integrated
             luminosity of 20.3 fb[Formula: see text], is used. Based on
             a new reconstruction algorithm used in 2012, the electron
             reconstruction efficiency is 97% for electrons with
             [Formula: see text] [Formula: see text] and 99% at
             [Formula: see text] [Formula: see text]. Combining this
             with the efficiency of additional selection criteria to
             reject electrons from background processes or misidentified
             hadrons, the efficiency to reconstruct and identify
             electrons at the ATLAS experiment varies from 65 to 95%,
             depending on the transverse momentum of the electron and
             background rejection.},
   Doi = {10.1140/epjc/s10052-017-4756-2},
   Key = {fds347495}
}

@article{fds307750,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Electron performance measurements with the ATLAS detector
             using the 2010 LHC proton-proton collision
             data},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {3},
   Pages = {1-46},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-1909-1},
   Abstract = {Detailed measurements of the electron performance of the
             ATLAS detector at the LHC are reported, using decays of the
             Z, W and J/ψ particles. Data collected in 2010 at √s = 7
             TeV are used, corresponding to an integrated luminosity of
             almost 40 pb-1. The inter-alignment of the inner detector
             and the electromagnetic calorimeter, the determination of
             the electron energy scale and resolution, and the
             performance in terms of response uniformity and linearity
             are discussed. The electron identification, reconstruction
             and trigger efficiencies, as well as the charge
             misidentification probability, are also presented. © 2012
             CERN for the benefit of the ATLAS collaboration.},
   Doi = {10.1140/epjc/s10052-012-1909-1},
   Key = {fds307750}
}

@article{fds310386,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
             J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov,
             A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
             M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau,
             M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
             P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Costa, JBGD and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
             N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji,
             W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and De Mendizabal,
             JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm,
             J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet,
             NM and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov,
             G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Renstrom, PABD and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Calvet, D and Calvet, S and Toro, RC and Camarda, S and Cameron, D and Caminada, LM and Armadans, RC and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cantero, J and Cantrill,
             R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Barajas, CAC and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
             IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland,
             W},
   Title = {Electron reconstruction and identification efficiency
             measurements with the ATLAS detector using the 2011 LHC
             proton-proton collision data.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {7},
   Pages = {2941},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-2941-0},
   Abstract = {Many of the interesting physics processes to be measured at
             the LHC have a signature involving one or more isolated
             electrons. The electron reconstruction and identification
             efficiencies of the ATLAS detector at the LHC have been
             evaluated using proton-proton collision data collected in
             2011 at [Formula: see text] TeV and corresponding to an
             integrated luminosity of 4.7 fb[Formula: see text].
             Tag-and-probe methods using events with leptonic decays of
             [Formula: see text] and [Formula: see text] bosons and
             [Formula: see text] mesons are employed to benchmark these
             performance parameters. The combination of all measurements
             results in identification efficiencies determined with an
             accuracy at the few per mil level for electron transverse
             energy greater than 30 GeV.},
   Doi = {10.1140/epjc/s10052-014-2941-0},
   Key = {fds310386}
}

@article{fds349790,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
             VA and Pereira, RA and Arce, ATH and Ardell, RE and Arduh,
             FA},
   Title = {Electron reconstruction and identification in the ATLAS
             experiment using the 2015 and 2016 LHC proton–proton
             collision data at √s=13 TeV},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {8},
   Year = {2019},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7140-6},
   Abstract = {Algorithms used for the reconstruction and identification of
             electrons in the central region of the ATLAS detector at the
             Large Hadron Collider (LHC) are presented in this paper;
             these algorithms are used in ATLAS physics analyses that
             involve electrons in the final state and which are based on
             the 2015 and 2016 proton–proton collision data produced by
             the LHC at s = 13 TeV. The performance of the electron
             reconstruction, identification, isolation, and charge
             identification algorithms is evaluated in data and in
             simulated samples using electrons from Z→ ee and J/ ψ→
             ee decays. Typical examples of combinations of electron
             reconstruction, identification, and isolation operating
             points used in ATLAS physics analyses are
             shown.},
   Doi = {10.1140/epjc/s10052-019-7140-6},
   Key = {fds349790}
}

@article{fds362158,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
             BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
             MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei,
             D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arguin, JF},
   Title = {Emulating the impact of additional proton–proton
             interactions in the ATLAS simulation by presampling sets of
             inelastic Monte Carlo events},
   Journal = {Computing and Software for Big Science},
   Volume = {6},
   Number = {1},
   Year = {2022},
   Month = {December},
   url = {http://dx.doi.org/10.1007/s41781-021-00062-2},
   Abstract = {The accurate simulation of additional interactions at the
             ATLAS experiment for the analysis of proton–proton
             collisions delivered by the Large Hadron Collider presents a
             significant challenge to the computing resources. During the
             LHC Run 2 (2015–2018), there were up to 70 inelastic
             interactions per bunch crossing, which need to be accounted
             for in Monte Carlo (MC) production. In this document, a new
             method to account for these additional interactions in the
             simulation chain is described. Instead of sampling the
             inelastic interactions and adding their energy deposits to a
             hard-scatter interaction one-by-one, the inelastic
             interactions are presampled, independent of the hard
             scatter, and stored as combined events. Consequently, for
             each hard-scatter interaction, only one such presampled
             event needs to be added as part of the simulation chain. For
             the Run 2 simulation chain, with an average of 35
             interactions per bunch crossing, this new method provides a
             substantial reduction in MC production CPU needs of around
             20%, while reproducing the properties of the reconstructed
             quantities relevant for physics analyses with good
             accuracy.},
   Doi = {10.1007/s41781-021-00062-2},
   Key = {fds362158}
}

@article{fds347524,
   Author = {Dewan, E and Biswas, D and Kakati, B and Verma, SK and Kotwal, A and Oberoi, A},
   Title = {Epidemiological and mycological characteristics of
             candidemia in patients with hematological malignancies
             attending a tertiary-care center in India.},
   Journal = {Hematology/oncology and stem cell therapy},
   Volume = {8},
   Number = {3},
   Pages = {99-105},
   Year = {2015},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.hemonc.2015.06.006},
   Abstract = {<h4>Background and objectives</h4>We undertook the present
             study to ascertain the contributing risk factors and explore
             the epidemiological and mycological characteristics of
             opportunistic candidemia among patients with hematological
             malignancies.<h4>Design and settings</h4>Observational
             cross-sectional study in a tertiary care center.<h4>Patients
             and methods</h4>Consecutive patients with hematological
             malignancies reporting to the collaborating medical and
             pediatric units with a febrile episode were recruited and
             screened for candidemia by blood culture. Recovered Candida
             isolates were speciated and antifungal susceptibility
             testing was performed as per Clinical and Laboratory
             Standards Institute guideline (CLSI) guidelines M44-A.
             Further analysis was done for potential risk factors and
             compared between culture positive and negative
             patients.<h4>Results</h4>Of 150 patients recruited, the
             majority (n=27) were between 51 and 60 years and the male to
             female ratio was 1.63:1. Fifteen patients (10%) were culture
             positive. The culture positivity was significantly higher in
             acute lymphocytic leukemia (ALL) than in non-ALL patients
             (p=0.03). There was significant association of candidaemia
             with leucopenia, chemotherapeutic drugs, corticosteroids and
             presence of indwelling devices. Duration of disease
             (p=0.032) and duration of hospitalization (p=0.003) were
             significantly prolonged in culture positive patients. C.
             tropicalis was the commonest isolate (46.67%), with non-
             Candida albicans outnumbering C. albicans in all categories
             of hematological malignancies (2.75:1). All isolates of C.
             albicans were uniformly sensitive to all the azoles, but
             only 50% were sensitive to amphotericin B and none to
             nystatin and flucytosine.<h4>Conclusions</h4>This
             observational study identifies ALL and chronic lymphocytic
             leukemia (CLL) as the forms of hematological malignancy
             predominantly associated with candidemia; specifies risk
             factors and chemotherapeutic agents predisposing patients
             towards its occurrence; reports a preponderance of C.
             tropicalis among the causative agents and finds voriconazole
             to be the most effective antifungal agent against the
             recovered isolates. This information could assist in
             tailoring prophylactic and therapeutic antifungal practices
             for this infection, according to local epidemiological and
             mycological characteristics.},
   Doi = {10.1016/j.hemonc.2015.06.006},
   Key = {fds347524}
}

@article{fds313598,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Erratum : Measurement of the inclusive jet cross-section in
             proton-proton collisions at √s = 7 TeV using 4.5
             fb−1 of data with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {9},
   Pages = {1-39},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2015)141},
   Abstract = {Abstract: It was found that the non-perturbative corrections
             calculated using Pythia with the Perugia 2011 tune did not
             include the effect of the underlying event. The affected
             correction factors were recomputed using the Pythia 6.427
             generator. These corrections are applied as baseline to the
             NLO pQCD calculations and thus the central values of the
             theoretical predictions have changed by a few percent with
             the new corrections. This has a minor impact on the
             agreement between the data and the theoretical predictions.
             Figures 2 and 6 to 13, and all the tables have been updated
             with the new values. A few sentences in the discussion in
             sections 5.2 and 9 were altered or removed.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP09(2015)141},
   Key = {fds313598}
}

@article{fds314798,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Erratum to ATLAS Run 1 searches for direct pair production
             of third-generation squarks at the Large Hadron
             Collider},
   Journal = {European Physical Journal C},
   Volume = {76},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {March},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-3935-x},
   Doi = {10.1140/epjc/s10052-016-3935-x},
   Key = {fds314798}
}

@article{fds307774,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M},
   Title = {Erratum to: "Search for first generation scalar leptoquarks
             in pp collisions at s=7TeV with the ATLAS detector" [Phys.
             Lett. B 709 (2012) 158]},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {711},
   Number = {5},
   Pages = {442-455},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.03.023},
   Doi = {10.1016/j.physletb.2012.03.023},
   Key = {fds307774}
}

@article{fds376411,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
             MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
             CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA and Arcangeletti,
             C},
   Title = {Erratum to: Higgs boson production cross-section
             measurements and their EFT interpretation in the 4 ℓ decay
             channel at s = 13 TeV with the ATLAS detector (The European
             Physical Journal C, (2020), 80, 10, (957),
             10.1140/epjc/s10052-020-8227-9)},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {5},
   Year = {2021},
   Month = {May},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09116-6},
   Abstract = {When quoting the final cross section result in the text of
             the paper (Eur. Phys. J. C 80 (2020) 957), the theory
             component of the uncertainty was incorrectly set to 0.04 pb
             while the correct value of 0.03 pb was given in Table 8 and
             in all other results reported in this paper.},
   Doi = {10.1140/epjc/s10052-021-09116-6},
   Key = {fds376411}
}

@article{fds355147,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
             MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
             CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA and Arcangeletti,
             C},
   Title = {Erratum to: Higgs boson production cross-section
             measurements and their EFT interpretation in the 4 ℓ decay
             channel at s = 13 TeV with the ATLAS detector (The European
             Physical Journal C, (2020), 80, 10, (957),
             10.1140/epjc/s10052-020-8227-9)},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {1},
   Year = {2021},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-08644-x},
   Abstract = {In the published HTML version of this article, the
             affiliations of the authors of the National Research Nuclear
             University MEPhI, Moscow, Russia were unfortunately marked
             incorrectly.},
   Doi = {10.1140/epjc/s10052-020-08644-x},
   Key = {fds355147}
}

@article{fds353482,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
             V},
   Title = {Erratum to: Measurement of differential cross sections for
             single diffractive dissociation in s = 8 TeV pp collisions
             using the ATLAS ALFA spectrometer (Journal of High Energy
             Physics, (2020), 2020, 2, (42), 10.1007/JHEP02(2020)042)},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {10},
   Year = {2020},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2020)182},
   Abstract = {The ATLAS collaboration E-mail: atlas.publications@cern.ch
             Erratum to: JHEP02(2020)042 ArXiv ePrint: 1911.00453 Figure
             5b of the paper [1] contained a misinterpretation in the
             comparison between the reported new ATLAS measurement of the
             process pp ! Xp and previously published CMS data [2]. The
             ATLAS measurement corresponds to cases where either proton
             dissociates. In the comparison, the CMS measurement was
             assumed to be defined similarly, whereas in fact it includes
             the dissociation of only one of the protons. On further
             investigation, the comparison between the ATLAS and CMS
             measurements is far from straightforward. The double
             dissociation (pp → XY ) contribution in the CMS data is
             not well constrained and indications from the CMS analysis
             suggest it may be significantly larger than was thought
             originally. Fuerthermore, the potentially sizeable central
             diffraction (pp → pXp) contribution was subtracted in the
             ATLAS measurement, but included by CMS. There is also a
             small effect associated with the different centre of mass
             energies (7 TeV for CMS and 8 TeV for ATLAS). In view of
             these complications, the figure has now been withdrawn from
             the publication [1].},
   Doi = {10.1007/JHEP10(2020)182},
   Key = {fds353482}
}

@article{fds361872,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R},
   Title = {Erratum to: Measurement of hadronic event shapes in high-p
             T multijet final states at s = 13 TeV with the
             ATLAS detector (Journal of High Energy Physics, (2021),
             2021, 1, (188), 10.1007/JHEP01(2021)188)},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {12},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2021)053},
   Abstract = {An error in the normalization of the Aplanarity and
             D-parameter has been found. Insufficient precision on the
             eigenvalue calculation can cause λ3 to be negative,
             exclusively in two-jet events, yielding an underestimation
             of the inclusive two-jet cross section.},
   Doi = {10.1007/JHEP12(2021)053},
   Key = {fds361872}
}

@article{fds359999,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R},
   Title = {Erratum to: Measurement of light-by-light scattering and
             search for axion-like particles with 2.2 nb −1
             of Pb+Pb data with the ATLAS detector (Journal of High
             Energy Physics, (2021), 2021, 3, (243), 10.1007/JHEP03(2021)243)},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {11},
   Year = {2021},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2021)050},
   Abstract = {One correction is noted for the paper, which does not affect
             the results reported. The right panel of figure 9 is
             corrected as it contained the “internal” label, giving
             the misleading impression on the credibility of the
             figure.},
   Doi = {10.1007/JHEP11(2021)050},
   Key = {fds359999}
}

@article{fds347447,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
             H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
             A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti,
             M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
             J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho,
             J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
             Alberich, L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan,
             SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont,
             AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
   Title = {Erratum to: Measurement of the W boson polarisation
             in t t ¯ events from pp collisions at s = 8 TeV in
             the lepton + jets channel with ATLAS.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {79},
   Number = {1},
   Pages = {19},
   Year = {2019},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-6520-7},
   Abstract = {[This corrects the article DOI: 10.1140/epjc/s10052-017-4819-4.].},
   Doi = {10.1140/epjc/s10052-018-6520-7},
   Key = {fds347447}
}

@article{fds356746,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Erratum to: Measurement of the charge asymmetry in top-quark
             pair production in the lepton-plus-jets final state in pp
             collision data at √s = 8 TeV with the ATLAS detector (The
             European Physical Journal C, (2016), 76, 2, (87),
             10.1140/epjc/s10052-016-3910-6)},
   Journal = {European Physical Journal C},
   Volume = {77},
   Number = {8},
   Year = {2017},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5089-x},
   Abstract = {In the original paper, Fig. 4 contains the wrong label
             preliminary. The label has been fixed, while none of the
             results have changed.(Table Presented.).},
   Doi = {10.1140/epjc/s10052-017-5089-x},
   Key = {fds356746}
}

@article{fds356644,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
             M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Erratum to: Measurement of the W-boson mass in pp collisions
             at √s=7 TeV with the ATLAS detector (The European Physical
             Journal C, (2018), 78, 2, (110), 10.1140/epjc/s10052-017-5475-4)},
   Journal = {European Physical Journal C},
   Volume = {78},
   Number = {11},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-6354-3},
   Abstract = {It has been found that Figure 30 shows the 68% and 99%
             confidence-level contours for the W boson and top quark mass
             measurements, instead of the 68% and 95% confidence-level
             contours, as stated in the legend.},
   Doi = {10.1140/epjc/s10052-018-6354-3},
   Key = {fds356644}
}

@article{fds354097,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
             JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
             VA},
   Title = {Erratum to: Measurements of top-quark pair differential and
             double-differential cross-sections in the ℓ +jets channel
             with pp collisions at s = 13 TeV using the ATLAS detector
             [Eur. Phys. J. C 79 (2019) 1028] (The European Physical
             Journal C, (2019), 79, 12, (1028), 10.1140/epjc/s10052-019-7525-6)},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {11},
   Year = {2020},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-08541-3},
   Abstract = {Corrections for five figures and six tables are noted for
             the paper, which do not affect the conclusions
             reported.},
   Doi = {10.1140/epjc/s10052-020-08541-3},
   Key = {fds354097}
}

@article{fds356599,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos, SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella, L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Erratum to: Measurements of W and Z boson production in pp
             collisions at s = 5.02 TeV with the ATLAS detector (The
             European Physical Journal C, (2019), 79, 2, (128),
             10.1140/epjc/s10052-019-6622-x)},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {5},
   Year = {2019},
   Month = {May},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-6870-9},
   Abstract = {It has been found that the theoretical predictions for W and
             Z boson cross sections, and for the W boson charge
             asymmetry, which are labelled as NNPDF3.1 [1] have in fact
             been calculated using the NNPDF3.0 PDF set [2]
             instead.},
   Doi = {10.1140/epjc/s10052-019-6870-9},
   Key = {fds356599}
}

@article{fds350335,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
             V},
   Title = {Erratum to: Search for diboson resonances in hadronic final
             states in 139 fb −1 of pp collisions at s = 13
             TeV with the ATLAS detector (Journal of High Energy Physics,
             (2019), 2019, 9, (91), 10.1007/JHEP09(2019)091)},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {6},
   Year = {2020},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2020)042},
   Abstract = {A mistake was identified for the paper [1] in the treatment
             of the radion [2] cross-sections, which resulted in multiple
             changes.},
   Doi = {10.1007/JHEP06(2020)042},
   Key = {fds350335}
}

@article{fds356645,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Erratum to: Search for heavy resonances decaying into a W or
             Z boson and a Higgs boson in final states with leptons and
             b-jets in 36 fb−1 of √s = 13 TeV pp
             collisions with the ATLAS detector (Journal of High Energy
             Physics, (2018), 2018, 3, (174), 10.1007/JHEP03(2018)174)},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {11},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2018)051},
   Abstract = {One correction is noted for the paper. The exclusion limits
             for the gluon-gluon fusion production of an A boson reported
             in the conclusions did not correspond to the exclusion plots
             shown in figure 6a.},
   Doi = {10.1007/JHEP11(2018)051},
   Key = {fds356645}
}

@article{fds310261,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Erratum to: Search for new phenomena in final states with an
             energetic jet and large missing transverse momentum in pp
             collisions at √s=8 TeV with the ATLAS detector (Eur. Phys.
             J. C (2015) 75:299, 10.1140/epjc/s10052-015-3517-3)},
   Journal = {European Physical Journal C},
   Volume = {75},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {September},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3639-7},
   Doi = {10.1140/epjc/s10052-015-3639-7},
   Key = {fds310261}
}

@article{fds355666,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
             KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
   Title = {Erratum to: Search for phenomena beyond the Standard Model
             in events with large b-jet multiplicity using the ATLAS
             detector at the LHC (The European Physical Journal C,
             (2021), 81, 1, (11), 10.1140/epjc/s10052-020-08730-0)},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {3},
   Year = {2021},
   Month = {March},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-08970-8},
   Abstract = {In the original HTML version of this article, one
             affiliation of the author V. O. Tikhomirov was missing. He
             is affiliated to the following two affiliations: P.N.
             Lebedev Physical Institute of the Russian Academy of
             Sciences, Moscow, Russia National Research Nuclear
             University MEPhI, Moscow, Russia The original article has
             been corrected.},
   Doi = {10.1140/epjc/s10052-021-08970-8},
   Key = {fds355666}
}

@article{fds359797,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
             C},
   Title = {Erratum to: Search for squarks and gluinos in final states
             with one isolated lepton, jets, and missing transverse
             momentum at √s = 13 TeV with the ATLAS detector (The
             European Physical Journal C, (2021), 81, 7, (600),
             10.1140/epjc/s10052-021-09344-w)},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {10},
   Year = {2021},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09748-8},
   Abstract = {In this article the title was incorrectly given as ‘Search
             for squarks and gluinos in final states with one isolated
             lepton, jets, and missing transverse momentum at √s = 13
             with the ATLAS detector’ but should have been ‘Search
             for squarks and gluinos in final states with one isolated
             lepton, jets, and missing transverse momentum at √s = 13
             TeV with the ATLAS detector’. The original article has
             been corrected.},
   Doi = {10.1140/epjc/s10052-021-09748-8},
   Key = {fds359797}
}

@article{fds313600,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Piqueras, DÁ and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Erratum to: Search for supersymmetry in events containing a
             same-flavour opposite-sign dilepton pair, jets, and large
             missing transverse momentum in √s = 8 TeV pp collisions
             with the ATLAS detector (Eur. Phys. J. C, (2015), 75, (318),
             10.1140/epjc/s10052-015-3518-2)},
   Journal = {European Physical Journal C},
   Volume = {75},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {October},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3661-9},
   Doi = {10.1140/epjc/s10052-015-3661-9},
   Key = {fds313600}
}

@article{fds314799,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Erratum to: Study of the spin and parity of the Higgs boson
             in diboson decays with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {76},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {March},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-3934-y},
   Doi = {10.1140/epjc/s10052-016-3934-y},
   Key = {fds314799}
}

@article{fds307567,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Erratum: Indirect measurement of sin-W
             (MW) using e+e - pairs in
             the Z-boson region with pp̄ collisions at a
             center-of-momentum energy of 1.96 TeV (Physical Review D
             (2013) 88 (072002))},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.079905},
   Doi = {10.1103/PhysRevD.88.079905},
   Key = {fds307567}
}

@article{fds352893,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
             P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Erratum: Measurement of differential cross sections and W
             + /W  cross-section ratios for W
             boson production in association with jets at s = 8 TeV with
             the ATLAS detector (Journal of High Energy Physics, (2018),
             2018, 5, (77), 10.1007/JHEP05(2018)077)},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {10},
   Year = {2020},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2020)048},
   Abstract = {Two additions impacting tables 3 and 4 in ref. [1] are
             presented in the following. No significant impact is found
             for other results or figures in ref. [1].},
   Doi = {10.1007/JHEP10(2020)048},
   Key = {fds352893}
}

@article{fds307917,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D},
   Title = {Erratum: Measurement of particle production and inclusive
             differential cross sections in pp̄ collisions at
             √s=1.96TeV (Physical Review D - Particles, Fields,
             Gravitation and Cosmology)},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {82},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.119903},
   Doi = {10.1103/PhysRevD.82.119903},
   Key = {fds307917}
}

@article{fds307968,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
             F and Bednar, P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
             A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
             A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli,
             M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi,
             R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G},
   Title = {Erratum: Measurement of the inclusive jet cross section at
             the Fermilab Tevatron pp̄ collider using a cone-based jet
             algorithm (Physical Review D (2008) 78 (052006))},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.119902},
   Doi = {10.1103/PhysRevD.79.119902},
   Key = {fds307968}
}

@article{fds308076,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
             M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
             MA},
   Title = {Erratum: Measurement of the inclusive jet cross section
             using the kT algorithm in pp̄ collisions at s=1.96TeV with
             the CDF II detector (Physical Review D - Particles, Fields,
             Gravitation and Cosmology (2007) 75, (092006))},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {75},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.119901},
   Doi = {10.1103/PhysRevD.75.119901},
   Key = {fds308076}
}

@article{fds307919,
   Author = {Aaltonen, T and Adelman, J and Álvarez Gonzalez, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
             S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M},
   Title = {Erratum: Measurement of the W+W-
             production cross section and search for anomalous WWγ and
             WWZ couplings in pp̄ collisions at √s=1.96 TeV (Phys.
             Rev. Lett. (2010) 104 (201801))},
   Journal = {Physical Review Letters},
   Volume = {105},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.019905},
   Doi = {10.1103/PhysRevLett.105.019905},
   Key = {fds307919}
}

@article{fds307669,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'Errico, M},
   Title = {Erratum: Novel inclusive search for the Higgs boson in the
             four-lepton final state at CDF (Physical Review D (2012) 86
             (072012) DOI:10.1103/PhysRevD. 86.072012)},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {9},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.099902},
   Doi = {10.1103/PhysRevD.86.099902},
   Key = {fds307669}
}

@article{fds308139,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
             J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
             J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH},
   Title = {Erratum: Search for Bs0 → μ+μ and Bd0 → μ+μ decays
             in pp_ collisions with CDF II (Phys. Rev. Lett. (2005) 95
             (221805))},
   Journal = {Physical Review Letters},
   Volume = {95},
   Number = {24},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevLett.95.249905},
   Doi = {10.1103/PhysRevLett.95.249905},
   Key = {fds308139}
}

@article{fds336454,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Erratum: Search for Bs0 →μ+μ- and B0 →μ+μ- decays
             with the full CDF Run II data set (Physical Review D (2013)
             87 (072003) DOI: 10.1103/PhysRevD.87.072003)},
   Journal = {Physical Review D},
   Volume = {97},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2018},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.97.099901},
   Abstract = {V. Krutelyov, of Texas A&M University and the University of
             California at Santa Barbara, was erroneously omitted from
             the author list.},
   Doi = {10.1103/PhysRevD.97.099901},
   Key = {fds336454}
}

@article{fds329967,
   Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'Orso, M and Deluca,
             C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico,
             M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati,
             S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
             JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
             MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
             MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
             E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Sperka, D and Squillacioti, P and Stancari, M and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang, YC},
   Title = {Erratum: Search for Bs0→μ+μ- and
             B0→μ+μ- decays with CDF II
             (Physical Review Letters (2011) 107 (191801))},
   Journal = {Physical Review Letters},
   Volume = {107},
   Number = {23},
   Year = {2011},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.239903},
   Doi = {10.1103/PhysRevLett.107.239903},
   Key = {fds329967}
}

@article{fds307973,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
             F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley,
             M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell,
             M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A},
   Title = {Erratum: Search for high-mass e+e- Resonances in pp̄
             collisions at s=1.96TeV (Physical Review Letters (2009) 102
             (031801))},
   Journal = {Physical Review Letters},
   Volume = {102},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevLett.102.059901},
   Doi = {10.1103/PhysRevLett.102.059901},
   Key = {fds307973}
}

@article{fds355986,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C},
   Title = {Erratum: Search for new non-resonant phenomena in high-mass
             dilepton final states with the ATLAS detector (Journal of
             High Energy Physics, (2020), 2020, 11, (5),
             10.1007/JHEP11(2020)005)},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {4},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2021)142},
   Abstract = {The Lagrangian in eq. (2.1) of JHEP11 (2020) 005 has an
             erroneous factor of 1/2. The analysis code used for the
             results reported in the paper does not have this factor. The
             results remain unchanged.},
   Doi = {10.1007/JHEP04(2021)142},
   Key = {fds355986}
}

@article{fds307555,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Erratum: Search for new phenomena in final states with large
             jet multiplicities and missing transverse momentum at √s =
             8 TeV proton-proton collisions using the ATLAS experiment
             (Journal of High Energy Physics (2013) 10
             (130))},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2014)109},
   Doi = {10.1007/JHEP01(2014)109},
   Key = {fds307555}
}

@article{fds308030,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             Gonzalez, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
   Title = {Erratum: Search for pair production of scalar top quarks
             decaying to a τ Lepton and a b quark in pp̄ collisions at
             s=1.96TeV (Physical Review Letters (2008) 101
             (071802))},
   Journal = {Physical Review Letters},
   Volume = {101},
   Number = {8},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevLett.101.089901},
   Doi = {10.1103/PhysRevLett.101.089901},
   Key = {fds308030}
}

@article{fds310266,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Ålkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Erratum: Search for production of WW/WZ resonances decaying
             to a lepton, neutrino and jets in pp collisions at √s = 8
             TeV with the ATLAS detector (The European Physical Journal C
             (2015) 75 (209) DOI: 10.1140/epjc/s10052-015-3425-6)},
   Journal = {European Physical Journal C},
   Volume = {75},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3593-4},
   Doi = {10.1140/epjc/s10052-015-3593-4},
   Key = {fds310266}
}

@article{fds351562,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
             J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri,
             A and Cerrito, L and Chapman, J and Chen, YC and Chertok, M and Chiarelli,
             G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chuang, S and Chung, K and Chung, WH and Chung, YS and Cijliak, M and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway,
             J},
   Title = {Erratum: Search for scalar leptoquark pairs decaying to
             ννqq in pp collisions at √(s)=1.96 TeV (Physical Review
             D (2005) 71 (112001) DOI: 10.1103/PhysRevD.71.112001)},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {11},
   Year = {2005},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.119901},
   Abstract = {This paper was published online on 2 June 2005 with a
             typographical error in the title. The title should read as
             "⋯ √s = 1:96 TeV." The title has been corrected as of 10
             June 2005. The title is correct in the printed version of
             the journal.},
   Doi = {10.1103/PhysRevD.71.119901},
   Key = {fds351562}
}

@article{fds356585,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Erratum: Search for supersymmetry in final states with two
             same-sign or three leptons and jets using 36
             fb−1 of s = 13 TeV pp collision data with the
             ATLAS detector (Journal of High Energy Physics, (2017),
             2017, 9, (84), 10.1007/JHEP09(2017)084)},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {8},
   Year = {2019},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2019)121},
   Abstract = {One correction is made to the figure 4e of the
             paper.},
   Doi = {10.1007/JHEP08(2019)121},
   Key = {fds356585}
}

@article{fds307573,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Guimaraes Da Costa and J and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger,
             J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
             J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz,
             D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Evidence for a bottom baryon resonance Λb*0 in CDF
             data},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {7},
   Pages = {071101},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.071101},
   Abstract = {Using data from proton-antiproton collisions at √s=1.96
             TeV recorded by the CDF II detector at the Fermilab
             Tevatron, evidence for the excited resonance state Λb*0 is
             presented in its Λb0π -π+ decay followed by the Λb0→Λ
             c+π- and Λc+→pK-π+ decays. The analysis is based on a
             data sample corresponding to an integrated luminosity of 9.6
             fb-1 collected by an online event selection based on
             charged-particle tracks displaced from the proton-antiproton
             interaction point. The significance of the observed signal
             is 3.5σ. The mass of the observed state is found to be
             5919.22±0.76 MeV/c2 in agreement with similar findings in
             proton-proton collision experiments. © 2013 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.88.071101},
   Key = {fds307573}
}

@article{fds307878,
   Author = {Aaltonen, and T, and al, E},
   Title = {Evidence for a mass dependent forward-backward asymmetry in
             top quark pair production},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {11},
   Pages = {112003},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.112003},
   Abstract = {We present a new measurement of the inclusive
             forward-backward tt̄ production asymmetry and its rapidity
             and mass dependence. The measurements are performed with
             data corresponding to an integrated luminosity of 5.3fb -1
             of pp̄ collisions at √s=1.96TeV, recorded with the CDF-II
             Detector at the Fermilab Tevatron. Significant inclusive
             asymmetries are observed in both the laboratory frame and
             the tt̄ rest frame, and in both cases are found to be
             consistent with CP conservation under interchange of t and
             t̄. In the tt̄ rest frame, the asymmetry is observed to
             increase with the tt̄ rapidity difference, Δy, and with
             the invariant mass M tt̄ of the tt̄ system. Fully
             corrected parton-level asymmetries are derived in two
             regions of each variable, and the asymmetry is found to be
             most significant at large Δy and Mtt̄. For
             Mtt̄?450GeV/c2, the parton-level asymmetry in the tt̄ rest
             frame is Att̄=0.475±0.114 compared to a next-to-leading
             order QCD prediction of 0.088±0.013. © 2011 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.83.112003},
   Key = {fds307878}
}

@article{fds307994,
   Author = {Aaltonen, T and others},
   Title = {Evidence for a Narrow Near-Threshold Structure in the J/ψϕ
             Mass Spectrum in B+→J/ψϕK+ Decays},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {24},
   Pages = {242002},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.242002},
   Abstract = {Evidence is reported for a narrow structure near the J/ψϕ
             threshold in exclusive B+→J/ψϕK+ decays produced in p̅
             p collisions at sqrt[s]=1.96  TeV. A signal of 14
             &plusmn; 5 events, with statistical significance in excess
             of 3.8 standard deviations, is observed in a data sample
             corresponding to an integrated luminosity of 2.7  fb-1,
             collected by the CDF II detector. The mass and natural width
             of the structure are measured to be 4143.0 &plusmn;
             2.9(stat) &plusmn; 1.2(syst)  MeV/c2 and
             11.7-5.0+8.3(stat) &plusmn; 3.7(syst)  MeV/c2.},
   Doi = {10.1103/physrevlett.102.242002},
   Key = {fds307994}
}

@article{fds307691,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Alvarez
             González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
             A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
             T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins,
             S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
             JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
             SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
             D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brown, J and Brucken, E and Budagov, J and Bu, XB and Budd, HS and Buehler,
             M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto,
             G and Bussey, P and Buszello, CP and Buzatu, A and Calamba, A and Calancha,
             C and Camacho-Pérez, E and Camarda, S and Campanelli, M and Campbell,
             M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo,
             S and Carron, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chakrabarti, S and Chakraborty, D and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok, M and Chevalier-Théry,
             S and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, DK and Cho,
             K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Chung, WH and Chung, YS and Cihangir, S and Ciocci, MA and Claes, D and Clark, A and Clarke, C and Clutter, J and Compostella, G and Convery, ME and Conway,
             J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox, CA and Cox, DJ and Crescioli, F and Croc, A and Cuevas, J and Culbertson, R and Cutts, D and Dagenhart, D and d'Ascenzo, N and Das, A and Datta, M and Davies, G and de Barbaro, P and de
             Jong, SJ and De La Cruz-Burelo and E and Déliot, F and Dell'orso, M and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov,
             SP and d'Errico, M and Desai, S and Deterre, C and Devaughan, K and Devoto,
             F and Di Canto and A and Di Ruzza and B and Diehl, HT and Diesburg, M and Ding,
             PF and Dittmann, JR and Dominguez, A and Donati, S and Dong, P and D'Onofrio, M and Dorigo, M and Dorigo, T and Dubey, A and Dudko, LV and Duggan, D and Duperrin, A and Dutt, S and Dyshkant, A and Eads, M and Ebina, K and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Evans, H and Evdokimov, A and Evdokimov, VN and Facini, G and Farrington, S and Feindt, M and Feng, L and Ferbel, T and Fernandez, JP and Ferrazza, C and Fiedler, F and Field, R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest, R and Fortner, M and Fox, H and Frank, MJ and Franklin, M and Freeman, JC and Fuess, S and Funakoshi, Y and Gallinaro, M and Garcia-Bellido, A and Garcia, JE and García-González, JA and García-Guerra, GA and Garfinkel, AF and Garosi, P and Gavrilov, V and Gay, P and Geng, W and Gerbaudo, D and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu,
             S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Golovanov, G and Gomez-Ceballos, G and Gomez, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Goussiou, A and Grannis, PD and Greder, S and Greenlee,
             H and Grenier, G and Grinstein, S and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald, MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hagopian, S and Hahn, SR and Haley, J and Halkiadakis, E and Hamaguchi, A and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, D and Hare, M and Harel, A and Harr, RF and Hatakeyama, K and Hauptman, JM and Hays, C and Hays, J and Head, T and Hebbeker, T and Heck, M and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hewamanage, S and Hildreth,
             MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen,
             B and Hogan, J and Hohlfeld, M and Hopkins, W and Horn, D and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeans, DT and Jeon, EJ and Jeong,
             MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere, A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung, AW and Junk, TR and Juste, A and Kaadze, K and Kajfasz, E and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kasper, PA and Kato, Y and Katsanos, I and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava,
             A and Kharzheev, YN and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YJ and Kim,
             YK and Kimura, N and Kirby, M and Kiselevich, I and Klimenko, S and Knoepfel, K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Krop,
             D and Kruse, M and Krutelyov, V and Kuhr, T and Kulikov, S and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lammers, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lebrun, P and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis, JD and Li, D and Li,
             H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Lin,
             C-J and Lindgren, M and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lubatti, HJ and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lysak, R and Lys, J and Maciel, AKA and Madar, R and Madrak,
             R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G},
   Title = {Evidence for a particle produced in association with weak
             bosons and decaying to a bottom-antibottom quark pair in
             higgs boson searches at the tevatron.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {7},
   Pages = {071804},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.109.071804},
   Abstract = {We combine searches by the CDF and D0 Collaborations for the
             associated production of a Higgs boson with a W or Z boson
             and subsequent decay of the Higgs boson to a
             bottom-antibottom quark pair. The data, originating from
             Fermilab Tevatron pp collisions at √s = 1.96 TeV,
             correspond to integrated luminosities of up to 9.7 fb(-1).
             The searches are conducted for a Higgs boson with mass in
             the range 100-150 GeV/c(2). We observe an excess of events
             in the data compared with the background predictions, which
             is most significant in the mass range between 120 and 135
             GeV/c(2). The largest local significance is 3.3 standard
             deviations, corresponding to a global significance of 3.1
             standard deviations. We interpret this as evidence for the
             presence of a new particle consistent with the standard
             model Higgs boson, which is produced in association with a
             weak vector boson and decays to a bottom-antibottom quark
             pair.},
   Doi = {10.1103/physrevlett.109.071804},
   Key = {fds307691}
}

@article{fds351561,
   Author = {Acosta, and D, and others},
   Title = {Evidence for B/s0 --> Phi Phi decay and measurements of
             branching ratio and A(CP) for B+ --> Phi
             K+},
   Journal = {Phys. Rev. Lett.},
   Volume = {95},
   Number = {3},
   Pages = {031801},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/physrevlett.95.031801},
   Abstract = {http://arxiv.org/abs/hep-ex/0502044},
   Doi = {10.1103/physrevlett.95.031801},
   Key = {fds351561}
}

@article{fds356536,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez
             Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {Evidence for electroweak production of two jets in
             association with a Zγ pair in pp collisions at s=13 TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {803},
   Year = {2020},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2020.135341},
   Abstract = {Evidence for electroweak production of two jets in
             association with a Zγ pair in s=13 TeV proton–proton
             collisions at the Large Hadron Collider is presented. The
             analysis uses data collected by the ATLAS detector in 2015
             and 2016 that corresponds to an integrated luminosity of
             36.1fb−1. Events that contain a Z boson candidate decaying
             leptonically into either e+e− or μ+μ−, a photon, and
             two jets are selected. The electroweak component is measured
             with observed and expected significances of 4.1 standard
             deviations. The fiducial cross-section for electroweak
             production is measured to be σZγjj−EW=7.8±2.0fb, in
             good agreement with the Standard Model prediction.},
   Doi = {10.1016/j.physletb.2020.135341},
   Key = {fds356536}
}

@article{fds310352,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baker,
             S and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, MF and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch,
             A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
             V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
             J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y},
   Title = {Evidence for electroweak production of W±W±jj in pp
             collisions at sqrt[s] = 8 TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {113},
   Number = {14},
   Pages = {141803},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.113.141803},
   Abstract = {This Letter presents the first study of W(±)W(±)jj,
             same-electric-charge diboson production in association with
             two jets, using 20.3 fb(-1) of proton-proton collision data
             at sqrt[s] = 8  TeV recorded by the ATLAS detector at
             the Large Hadron Collider. Events with two reconstructed
             same-charge leptons (e(±)e(±), e(±)μ(±), and
             μ(±)μ(±)) and two or more jets are analyzed. Production
             cross sections are measured in two fiducial regions, with
             different sensitivities to the electroweak and strong
             production mechanisms. First evidence for W(±)W(±)jj
             production and electroweak-only W(±)W(±)jj production is
             observed with a significance of 4.5 and 3.6 standard
             deviations, respectively. The measured production cross
             sections are in agreement with standard model predictions.
             Limits at 95% confidence level are set on anomalous quartic
             gauge couplings.},
   Doi = {10.1103/physrevlett.113.141803},
   Key = {fds310352}
}

@article{fds356735,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Evidence for light-by-light scattering in heavy-ion
             collisions with the ATLAS detector at the
             LHC},
   Journal = {Nature Physics},
   Volume = {13},
   Number = {9},
   Pages = {852-858},
   Year = {2017},
   Month = {September},
   url = {http://dx.doi.org/10.1038/nphys4208},
   Abstract = {Light-by-light scattering (γγ → γγ) is a
             quantum-mechanical process that is forbidden in the
             classical theory of electrodynamics. This reaction is
             accessible at the Large Hadron Collider thanks to the large
             electromagnetic field strengths generated by
             ultra-relativistic colliding lead ions. Using 480 μ1 of
             lead-lead collision data recorded at a centre-of-mass energy
             per nucleon pair of 5.02 TeV by the ATLAS detector, here we
             report evidence for light-by-light scattering. A total of 13
             candidate events were observed with an expected background
             of 2.6 ± 0.7 events. After background subtraction and
             analysis corrections, the fiducial cross-section of the
             process Pb + Pb (γγ) → Pb(∗) + Pb(∗)γγ,for photon
             transverse energy ET > 3GeV, photon absolute pseudorapidity
             |η| <2.4, diphoton invariant mass greater than 6GeV,
             diphoton transverse momentum lower than 2GeV and diphoton
             acoplanarity below 0.01, is measured to be 70 ± 24 (stat.)
             ±17 (syst.) nb, which is in agreement with the standard
             model predictions.},
   Doi = {10.1038/nphys4208},
   Key = {fds356735}
}

@article{fds307533,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
             JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
             A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
             C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
             L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Vázquez, F and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Evidence for s-channel single-top-quark production in events
             with one charged lepton and two jets at CDF.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {23},
   Pages = {231804},
   Year = {2014},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.112.231804},
   Abstract = {We report evidence for s-channel single-top-quark production
             in proton-antiproton collisions at center-of-mass energy
             sqrt[s] = 1.96 TeV using a data set that corresponds to an
             integrated luminosity of 9.4 fb(-1) collected by the
             Collider Detector at Fermilab. We select events consistent
             with the s-channel process including two jets and one
             leptonically decaying W boson. The observed significance is
             3.8 standard deviations with respect to the background-only
             prediction. Assuming a top-quark mass of 172.5 GeV/c(2), we
             measure the s-channel cross section to be 1.41(-0.42)(+0.44)
             pb.},
   Doi = {10.1103/physrevlett.112.231804},
   Key = {fds307533}
}

@article{fds356769,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Evidence for single top-quark production in the s-channel in
             proton–proton collisions at √s=8 TeV with the ATLAS
             detector using the Matrix Element Method},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {756},
   Pages = {228-246},
   Year = {2016},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.03.017},
   Abstract = {This Letter presents evidence for single top-quark
             production in the s-channel using proton–proton collisions
             at a centre-of-mass energy of 8 TeV with the ATLAS detector
             at the CERN Large Hadron Collider. The analysis is performed
             on events containing one isolated electron or muon, large
             missing transverse momentum and exactly two b-tagged jets in
             the final state. The analysed data set corresponds to an
             integrated luminosity of 20.3 fb−1. The signal is
             extracted using a maximum-likelihood fit of a discriminant
             which is based on the matrix element method and optimized in
             order to separate single-top-quark s-channel events from the
             main background contributions, which are top-quark pair
             production and W boson production in association with
             heavy-flavour jets. The measurement leads to an observed
             signal significance of 3.2 standard deviations and a
             measured cross-section of σs=4.8±0.8(stat.)−1.3+1.6(syst.)
             pb, which is consistent with the Standard Model expectation.
             The expected significance for the analysis is 3.9 standard
             deviations.},
   Doi = {10.1016/j.physletb.2016.03.017},
   Key = {fds356769}
}

@article{fds307794,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D},
   Title = {Evidence for the associated production of a W boson and a
             top quark in ATLAS at √s=7TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {716},
   Number = {1},
   Pages = {142-159},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.08.011},
   Abstract = {This Letter presents evidence for the associated production
             of a W boson and a top quark using 2.05 fb−1 of pp
             collision data at s=7TeV accumulated with the ATLAS detector
             at the LHC. The analysis is based on the selection of the
             dileptonic final states with events featuring two isolated
             leptons, electron or muon, with significant transverse
             missing momentum and at least one jet. An approach based on
             boosted decision trees has been developed to improve the
             discrimination of single top-quark Wt events from
             background. A template fit to the final classifier
             distributions is performed to determine the cross-section.
             The result is incompatible with the background-only
             hypothesis at the 3.3σ level, the expected sensitivity
             assuming the Standard Model production rate being 3.4σ. The
             corresponding cross-section is determined and found to be
             σWt=16.8±2.9 (stat)±4.9 (syst) pb, in good agreement with
             the Standard Model expectation. From this result the CKM
             matrix element |Vtb|=1.03−0.19+0.16 is derived assuming
             that the Wt production through |Vts| and |Vtd| is
             small.},
   Doi = {10.1016/j.physletb.2012.08.011},
   Key = {fds307794}
}

@article{fds356689,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
             M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O},
   Title = {Evidence for the associated production of the Higgs boson
             and a top quark pair with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {97},
   Number = {7},
   Year = {2018},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.97.072003},
   Abstract = {A search for the associated production of the Higgs boson
             with a top quark pair (ttH) is reported. The search is
             performed in multilepton final states using a data set
             corresponding to an integrated luminosity of 36.1 fb-1 of
             proton-proton collision data recorded by the ATLAS
             experiment at a center-of-mass energy s=13 TeV at the Large
             Hadron Collider. Higgs boson decays to WW∗, ττ, and
             ZZ∗ are targeted. Seven final states, categorized by the
             number and flavor of charged-lepton candidates, are examined
             for the presence of the Standard Model Higgs boson with a
             mass of 125 GeV and a pair of top quarks. An excess of
             events over the expected background from Standard Model
             processes is found with an observed significance of 4.1
             standard deviations, compared to an expectation of 2.8
             standard deviations. The best fit for the ttH production
             cross section is σ(ttH)=790-210+230 fb, in agreement with
             the Standard Model prediction of 507-50+35 fb. The
             combination of this result with other ttH searches from the
             ATLAS experiment using the Higgs boson decay modes to bb,
             γγ and ZZ∗→4, has an observed significance of 4.2
             standard deviations, compared to an expectation of 3.8
             standard deviations. This provides evidence for the ttH
             production mode.},
   Doi = {10.1103/PhysRevD.97.072003},
   Key = {fds356689}
}

@article{fds307820,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt,
             N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zucchelli, S and CDF Collaboration},
   Title = {Evidence for the charmless annihilation decay mode
             B(s)(0)→π(+)π(-).},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {21},
   Pages = {211803},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.211803},
   Abstract = {We search for annihilation decay modes of neutral b mesons
             into pairs of charmless charged hadrons with the upgraded
             Collider Detector at the Fermilab Tevatron. Using a data
             sample corresponding to 6 fb(-1) of integrated luminosity,
             we obtain the first evidence for the B(s)(0)→π(+)π(-)
             decay, with a significance of 3.7σ, and a measured
             branching ratio B(B(s)(0)→π(+)π(-))=(0.57±0.15(stat)±0.10(syst))×10(-6).
             A search for the B(0)→K(+)K(-) mode in the same sample
             yields a significance of 2.0σ, and a central value estimate
             B(B(0)→K(+)K(-))=(0.23±0.10(stat)±0.10(syst))×10(-6).},
   Doi = {10.1103/physrevlett.108.211803},
   Key = {fds307820}
}

@article{fds308102,
   Author = {Acosta, and D, and others},
   Title = {Evidence for the exclusive decay B/c+- --> J/psi pi+- and
             measurement of the mass of the B/c meson},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {8},
   Pages = {082002},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.082002},
   Abstract = {We report first evidence for a fully reconstructed decay
             mode of the B+/-_c meson in the channel B+/-_c --> J/psi
             pi++/-, with J/psi --> mu+ mu-. The analysis is based on an
             integrated luminosity of 360 pb-1 in p anti-p collisions at
             1.96 TeV center of mass energy collected by the Collider
             Detector at Fermilab. We observe 14.6 +/- 4.6 signal events
             with a background of 7.1 +/- 0.9 events, and a fit to the
             J/psi pi++/- mass spectrum yields a B+/-_c mass of 6285.7
             +/- 5.3 (stat) +/- 1.2 (syst) MeV/c2. The probability of a
             peak of this magnitude occurring by random fluctuation in
             the search region is estimated as 0.012\%.},
   Doi = {10.1103/physrevlett.96.082002},
   Key = {fds308102}
}

@article{fds356718,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Evidence for the H → bb decay with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {12},
   Pages = {1-69},
   Year = {2017},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2017)024},
   Abstract = {A search for the decay of the Standard Model Higgs boson
             into a bb pair when produced in association with a W or Z
             boson is performed with the ATLAS detector. The analysed
             data, corresponding to an integrated luminosity of 36.1
             fb-1, were collected in proton-proton collisions in Run 2 of
             the Large Hadron Collider at a centre-of-mass energy of
             13TeV. Final states containing zero, one and two charged
             leptons (electrons or muons) are considered, targeting the
             decays Z → νν, W → ℓν and Z → ℓℓ. For a Higgs
             boson mass of 125 GeV, an excess of events over the expected
             background from other Standard Model processes is found with
             an observed significance of 3.5 standard deviations,
             compared to an expectation of 3.0 standard deviations. This
             excess provides evidence for the Higgs boson decay into
             b-quarks and for its production in association with a vector
             boson. The combination of this result with that of the Run 1
             analysis yields a ratio of the measured signal events to the
             Standard Model expectation equal to 0.90 ±
             0.18(stat.)+0.21-0.19(syst.). Assuming the Standard Model
             production cross-section, the results are consistent with
             the value of the Yukawa coupling to b-quarks in the Standard
             Model.},
   Doi = {10.1007/JHEP12(2017)024},
   Key = {fds356718}
}

@article{fds375333,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye,
             T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal,
             A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja,
             S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh,
             B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
             SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
             CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Artoni,
             G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol,
             AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal,
             D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balakrishnan, V and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barel, MZ and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
             K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
             L and Bellerive, A and Bellos, P and Beloborodov, K and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann,
             E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhalla, NK and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Biryukov, S and Bisanz, T and Bisceglie, E and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borissov, G and Bortoletto,
             D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans,
             G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bulekov, O and Bullard, BA and Burdin, S and Burgard,
             CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey,
             PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev, AR and Cabrera Urbán and S and Cadamuro,
             L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace,
             N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
             JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cepaitis, V and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty,
             D and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili,
             B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
             Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
             J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
             A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark, A and Clark, PJ},
   Title = {Evidence for the Higgs Boson Decay to a Z Boson and a Photon
             at the LHC.},
   Journal = {Physical review letters},
   Volume = {132},
   Number = {2},
   Pages = {021803},
   Year = {2024},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.132.021803},
   Abstract = {The first evidence for the Higgs boson decay to a Z boson
             and a photon is presented, with a statistical significance
             of 3.4 standard deviations. The result is derived from a
             combined analysis of the searches performed by the ATLAS and
             CMS Collaborations with proton-proton collision datasets
             collected at the CERN Large Hadron Collider (LHC) from 2015
             to 2018. These correspond to integrated luminosities of
             around 140  fb^{-1} for each experiment, at a
             center-of-mass energy of 13 TeV. The measured signal yield
             is 2.2±0.7 times the standard model prediction, and agrees
             with the theoretical expectation within 1.9 standard
             deviations.},
   Doi = {10.1103/physrevlett.132.021803},
   Key = {fds375333}
}

@article{fds310293,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H},
   Title = {Evidence for the Higgs-boson Yukawa coupling to tau leptons
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {4},
   Pages = {1-74},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2015)117},
   Abstract = {Abstract: Results of a search for H → ττ decays are
             presented, based on the full set of proton-proton collision
             data recorded by the ATLAS experiment at the LHC during 2011
             and 2012. The data correspond to integrated luminosities of
             4.5 fb−1 and 20.3 fb−1 at centre-of-mass energies of
             √s = 7 TeV and √s = 8 TeV respectively. All combinations
             of leptonic (τ→ℓνν¯ with ℓ = e, μ) and hadronic
             (τ → hadrons ν) tau decays are considered. An excess of
             events over the expected background from other Standard
             Model processes is found with an observed (expected)
             significance of 4.5 (3.4) standard deviations. This excess
             provides evidence for the direct coupling of the recently
             discovered Higgs boson to fermions. The measured signal
             strength, normalised to the Standard Model expectation, of
             μ = 1. 43− 0.37+ 0.43 is consistent with the predicted
             Yukawa coupling strength in the Standard Model.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP04(2015)117},
   Key = {fds310293}
}

@article{fds356560,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
             J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {Evidence for the production of three massive vector bosons
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {798},
   Year = {2019},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.134913},
   Abstract = {A search for the production of three massive vector bosons
             in proton–proton collisions is performed using data at
             s=13 TeV recorded with the ATLAS detector at the Large
             Hadron Collider in the years 2015–2017, corresponding to
             an integrated luminosity of 79.8 fb−1. Events with two
             same-sign leptons ℓ (electrons or muons) and at least two
             reconstructed jets are selected to search for
             WWW→ℓνℓνqq. Events with three leptons without any
             same-flavour opposite-sign lepton pairs are used to search
             for WWW→ℓνℓνℓν, while events with three leptons
             and at least one same-flavour opposite-sign lepton pair and
             one or more reconstructed jets are used to search for
             WWZ→ℓνqqℓℓ. Finally, events with four leptons are
             analysed to search for WWZ→ℓνℓνℓℓ and
             WZZ→qqℓℓℓℓ. Evidence for the joint production of
             three massive vector bosons is observed with a significance
             of 4.1 standard deviations, where the expectation is 3.1
             standard deviations.},
   Doi = {10.1016/j.physletb.2019.134913},
   Key = {fds356560}
}

@article{fds307583,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and AbdelKhalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and AlconadaVerzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and AlvarezGonzalez, B and Alviggi, MG and Amako, K and AmaralCoutinho, Y and Amelung, C and Ammosov, VV and AmorDosSantos, SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and AperioBella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
             M},
   Title = {Evidence for the spin-0 nature of the Higgs boson using
             ATLAS data},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {726},
   Number = {1-3},
   Pages = {120-144},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.08.026},
   Abstract = {Studies of the spin and parity quantum numbers of the Higgs
             boson are presented, based on proton-proton collision data
             collected by the ATLAS experiment at the LHC. The Standard
             Model spin-parity JP=0+ hypothesis is compared with
             alternative hypotheses using the Higgs boson decays
             H→γγ, H→ZZ*→4ℓ and H→WW*→ℓνℓν, as well
             as the combination of these channels. The analysed dataset
             corresponds to an integrated luminosity of 20.7 fb-1
             collected at a centre-of-mass energy of s=8TeV. For the
             H→ZZ*→4ℓ decay mode the dataset corresponding to an
             integrated luminosity of 4.6 fb-1 collected at s=7TeV is
             included. The data are compatible with the Standard Model
             JP=0+ quantum numbers for the Higgs boson, whereas all
             alternative hypotheses studied in this Letter, namely some
             specific JP=0-, 1+, 1-, 2+ models, are excluded at
             confidence levels above 97.8%. This exclusion holds
             independently of the assumptions on the coupling strengths
             to the Standard Model particles and in the case of the JP=2+
             model, of the relative fractions of gluon-fusion and
             quark-antiquark production of the spin-2 particle. The data
             thus provide evidence for the spin-0 nature of the Higgs
             boson, with positive parity being strongly preferred. ©
             2013 CERN.},
   Doi = {10.1016/j.physletb.2013.08.026},
   Key = {fds307583}
}

@article{fds353614,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler,
             A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso,
             S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen,
             T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
   Title = {Evidence for tt¯ tt¯ production in the multilepton final
             state in proton–proton collisions at √s=13 TeV with the
             ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {11},
   Year = {2020},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-08509-3},
   Abstract = {A search is presented for four-top-quark production using an
             integrated luminosity of 139 fb- 1 of proton–proton
             collision data at a centre-of-mass energy of 13TeV collected
             by the ATLAS detector at the LHC. Events are selected if
             they contain a same-sign lepton pair or at least three
             leptons (electrons or muons). Jet multiplicity, jet flavour
             and event kinematics are used to separate signal from the
             background through a multivariate discriminant, and
             dedicated control regions are used to constrain the dominant
             backgrounds. The four-top-quark production cross section is
             measured to be 24-6+7 fb. This corresponds to an observed
             (expected) significance with respect to the background-only
             hypothesis of 4.3 (2.4) standard deviations and provides
             evidence for this process.},
   Doi = {10.1140/epjc/s10052-020-08509-3},
   Key = {fds353614}
}

@article{fds337202,
   Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'Orso, M and Deluca,
             C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico,
             M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati,
             S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
             JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
             MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
             MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum, W and Keung,
             J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
             M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, C and Liu, Q and Liu, T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Maksimovic, P and Malik, S and Manca, G and Manousakis-Katsikakis,
             A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson,
             ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin,
             F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and Denis,
             RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
             J and Thompson, GA and Thomson, E and Tipton, P and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán,
             J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka,
             J},
   Title = {Evidence for tt̄γ production and measurement of
             σtt̄γtt̄},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {84},
   Number = {3},
   Year = {2011},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.031104},
   Abstract = {Using data corresponding to 6.0fb-1 of pp̄ collisions at
             √s=1.96TeV collected by the CDF II detector, we present a
             cross section measurement of top-quark pair production with
             an additional radiated photon in the central region with 10
             GeV or more of transverse energy tt̄γ. The events are
             selected by looking for a lepton (ℓ or μ), a photon (γ),
             significant transverse momentum imbalance (ET), large total
             transverse energy, and three or more jets, with at least one
             identified as containing a b quark (b). Using an event
             selection optimized for the tt̄γ candidate sample, we also
             measure the cross section of tt̄ (σtt̄). We measure the
             tt̄γ cross section (σtt̄γ) to be 0.18±0.08pb, and the
             ratio of σtt̄γ to σtt̄ to be 0.024±0.009. We observe a
             probability of 0.0015 (3.0 standard deviations) of the
             background (non-tt̄γ events alone producing 30 events or
             more. © 2011 American Physical Society.},
   Doi = {10.1103/PhysRevD.84.031104},
   Key = {fds337202}
}

@article{fds308221,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
             M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
             HT and Diesburg, M and di Loreto, G and Draper, P and Ducros, Y and Dudko,
             LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
             VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
             OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T},
   Title = {Evidence of color coherence effects in W + jets events from
             pp collisions at √s = 1.8 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {464},
   Number = {1-2},
   Pages = {145-155},
   Publisher = {Elsevier BV},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1016/S0370-2693(99)01015-1},
   Abstract = {We report the results of a study of color coherence effects
             in pp collisions based on data collected by the DØ detector
             during the 1994-1995 run of the Fermilab Tevatron Collider,
             at a center of mass energy √s = 1.8 TeV. Initial-to-final
             state color interference effects are observed by examining
             particle distribution patterns in events with a W boson and
             at least one jet. The data are compared to Monte Carlo
             simulations with different color coherence implementations
             and to an analytic modified-leading-logarithm perturbative
             calculation based on the local parton-hadron duality
             hypothesis. © 1999 Published by Elsevier Science B.V. All
             rights reserved.},
   Doi = {10.1016/S0370-2693(99)01015-1},
   Key = {fds308221}
}

@article{fds373739,
   Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
             J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
             W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
             PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
             Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
             V and Arcangeletti, C and Arce, ATH},
   Title = {Evidence of off-shell Higgs boson production from ZZ
             leptonic decay channels and constraints on its total width
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {846},
   Year = {2023},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.138223},
   Abstract = {This Letter reports on a search for off-shell production of
             the Higgs boson using 139 fb−1 of pp collision data at s=
             13 TeV collected by the ATLAS detector at the Large Hadron
             Collider. The signature is a pair of Z bosons, with
             contributions from both the production and subsequent decay
             of a virtual Higgs boson and the interference of that
             process with other processes. The two observable final
             states are ZZ→4ℓ and ZZ→2ℓ2ν with ℓ=e or μ. In
             the ZZ→4ℓ final state, a dense Neural Network is used to
             enhance analysis sensitivity with respect to matrix
             element-based discrimination. The background-only hypothesis
             is rejected with an observed (expected) significance of 3.3
             (2.2) standard deviations, representing experimental
             evidence for off-shell Higgs boson production. Assuming that
             no new particles enter the production of the virtual Higgs
             boson, its total width can be deduced from the measurement
             of its off-shell production cross-section. The measured
             total width of the Higgs boson is 4.5−2.5+3.3 MeV, and the
             observed (expected) upper limit on the total width is found
             to be 10.5 (10.9) MeV at 95% confidence level.},
   Doi = {10.1016/j.physletb.2023.138223},
   Key = {fds373739}
}

@article{fds310271,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
             AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo,
             T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell,
             SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
             S},
   Title = {Evidence of Wγγ Production in pp Collisions at
             sqrt[s]=8  TeV and Limits on Anomalous Quartic Gauge
             Couplings with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {115},
   Number = {3},
   Pages = {031802},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.115.031802},
   Abstract = {This Letter reports evidence of triple gauge boson
             production pp→W(ℓν)γγ+X, which is accessible for the
             first time with the 8 TeV LHC data set. The fiducial cross
             section for this process is measured in a data sample
             corresponding to an integrated luminosity of
             20.3  fb^{-1}, collected by the ATLAS detector in 2012.
             Events are selected using the W boson decay to eν or μν
             as well as requiring two isolated photons. The measured
             cross section is used to set limits on anomalous quartic
             gauge couplings in the high diphoton mass
             region.},
   Doi = {10.1103/physrevlett.115.031802},
   Key = {fds310271}
}

@article{fds307898,
   Author = {Aaltonen, and T, and others},
   Title = {Exclusion of an Exotic Top Quark with -4/3 Electric Charge
             Using Soft Lepton Tagging},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {10},
   Pages = {101801},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.101801},
   Abstract = {We present a measurement of the electric charge of the top
             quark using pp collisions corresponding to an integrated
             luminosity of 2.7 fb(-1) at the CDF II detector. We
             reconstruct tt events in the lepton + jets final state. We
             use soft lepton taggers to determine the flavor of the b
             jets, which we use to reconstruct the top quark's electric
             charge and exclude an exotic top quark with -4/3 charge at
             95% confidence level. This is the strongest exclusion of the
             exotic charge scenario and the first to use soft leptons for
             this purpose.},
   Doi = {10.1103/PhysRevLett.105.101801},
   Key = {fds307898}
}

@article{fds307587,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bortoletto, D and Boudreau, J and Boveia,
             A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
             F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar,
             R},
   Title = {Exclusion of exotic top-like quarks with -4/3 electric
             charge using jet-charge tagging in single-lepton tt̄ events
             at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {3},
   Pages = {032003},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.032003},
   Abstract = {We report on a measurement of the top-quark electric charge
             in tt̄ events in which one W boson originating from the
             top-quark pair decays into leptons and the other into
             hadrons. The event sample was collected by the CDF II
             detector in √s=1.96 TeV proton-antiproton collisions and
             corresponds to 5.6 fb-1. We find the data to be consistent
             with the standard model and exclude the existence of an
             exotic quark with -4/3 electric charge and mass of the
             conventional top quark at the 99% confidence level. © 2013
             American Physical Society.},
   Doi = {10.1103/PhysRevD.88.032003},
   Key = {fds307587}
}

@booklet{Abbott98p,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
             V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
             C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
             P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
             MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
             G and Fisk, HE and Fisyak, Y and Flattum, E},
   Title = {Experimental search for chargino and neutralino production
             in supersymmetry models with a light gravitino},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {3},
   Pages = {442-447},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.442},
   Abstract = {We search for inclusive high ETdiphoton events with large
             missing transverse energy in pp¯collisions at s=1.8 TeV.
             Such events are expected from pair production of charginos
             and neutralinos within the framework of the minimal
             supersymmetric standard model with a light gravitino. No
             excess of events is observed. In that model, and assuming
             gaugino mass unification at the GUT scale, we obtain a 95%
             C.L. exclusion region in the supersymmetry parameter space
             and lower mass bounds of 150 GeV/c2for the lightest chargino
             and 77GeV/c2for the lightest neutralino. © 1998 American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.80.442},
   Key = {Abbott98p}
}

@booklet{Adams95a,
   Author = {Adams, MR and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dhawan, SK and Dietrich, FS and Dougherty, W and Dreyer, T and Eckardt,
             V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen, KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Hughes, VW and Jackson, HE and Jaffe, DE and Jancso, G and Jansen, DM and Jin, Z and Kaufman, S and Kennedy, RD and Kinney, ER and Kobrak, HG and Kotwal, AV and Kunori, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin,
             JG and Nickerson, RB and Novak, J and O'Day, S and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou, V and Pawlik, B and Pipkin,
             FM},
   Title = {Extraction of the Ratio Fn2/Fp2 from Muon-Deuteron and
             Muon-Proton Scattering at Small x and Q2.},
   Journal = {Physical review letters},
   Volume = {75},
   Number = {8},
   Pages = {1466-1470},
   Year = {1995},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.75.1466},
   Doi = {10.1103/physrevlett.75.1466},
   Key = {Adams95a}
}

@article{fds308200,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evans, H and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk,
             HE and Fisyak, Y and Flattum, E},
   Title = {Extraction of the width of the W boson from measurements of
             [formula presented] and [formula presented] and their
             ratio},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {61},
   Number = {7},
   Pages = {1-22},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.61.072001},
   Abstract = {We report on measurements on inclusive cross sections times
             branching fractions into electrons for W and Z bosons
             produced in (Formula presented) collisions at (Formula
             presented) From an integrated luminosity of 84.5 (Formula
             presented) recorded in 1994–1995 using the DØ detector at
             the Fermilab Tevatron, we determine (Formula presented) and
             (Formula presented) From these, we derive (Formula
             presented) (Formula presented) and (Formula presented) We
             use the latter to set a 95% confidence level upper limit on
             the partial decay width of the W boson into nonstandard
             model final states, (Formula presented) of 0.213 GeV.
             Combining these results with those from the 1992–1993 data
             gives (Formula presented) (Formula presented) and a 95% C.L.
             upper limit on (Formula presented) of 0.191 GeV. Using a
             sample with a luminosity of 505 (Formula presented) taken at
             (Formula presented) we measure (Formula presented) © 2000
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.61.072001},
   Key = {fds308200}
}

@article{fds374916,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
             SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Aly, M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
             CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
   Title = {Fast b-tagging at the high-level trigger of the ATLAS
             experiment in LHC Run 3},
   Journal = {Journal of Instrumentation},
   Volume = {18},
   Number = {11},
   Year = {2023},
   Month = {November},
   url = {http://dx.doi.org/10.1088/1748-0221/18/11/P11006},
   Abstract = {The ATLAS experiment relies on real-time hadronic jet
             reconstruction and b-tagging to record fully hadronic events
             containing b-jets. These algorithms require track
             reconstruction, which is computationally expensive and could
             overwhelm the high-level-trigger farm, even at the reduced
             event rate that passes the ATLAS first stage hardware-based
             trigger. In LHC Run 3, ATLAS has mitigated these
             computational demands by introducing a fast
             neural-network-based b-tagger, which acts as a low-precision
             filter using input from hadronic jets and tracks. It runs
             after a hardware trigger and before the remaining
             high-level-trigger reconstruction. This design relies on the
             negligible cost of neural-network inference as compared to
             track reconstruction, and the cost reduction from limiting
             tracking to specific regions of the detector. In the case of
             Standard Model HH → bb̄bb̄, a key signature relying on
             b-jet triggers, the filter lowers the input rate to the
             remaining high-level trigger by a factor of five at the
             small cost of reducing the overall signal efficiency by
             roughly 2%.},
   Doi = {10.1088/1748-0221/18/11/P11006},
   Key = {fds374916}
}

@article{fds356591,
   Author = {Abada, A and Abbrescia, M and AbdusSalam, SS and Abdyukhanov, I and Fernandez, JA and Abramov, A and Aburaia, M and Acar, AO and Adzic, PR and Agrawal, P and Aguilar-Saavedra, JA and Aguilera-Verdugo, JJ and Aiba, M and Aichinger, I and Aielli, G and Akay, A and Akhundov, A and Aksakal, H and Albacete, JL and Albergo, S and Alekou, A and Aleksa, M and Aleksan, R and Fernandez, RMA and Alexahin, Y and Alía, RG and Alioli,
             S and Tehrani, NA and Allanach, BC and Allport, PP and Altınlı, M and Altmannshofer, W and Ambrosio, G and Amorim, D and Amstutz, O and Anderlini, L and Andreazza, A and Andreini, M and Andriatis, A and Andris, C and Andronic, A and Angelucci, M and Antinori, F and Antipov,
             SA and Antonelli, M and Antonello, M and Antonioli, P and Antusch, S and Anulli, F and Apolinário, L and Apollinari, G and Apollonio, A and Appelö, D and Appleby, RB and Apyan, A and Arbey, A and Arbuzov, A and Arduini, G and Arı, V and Arias, S and Armesto, N and Arnaldi, R and Arsenyev, SA and Arzeo, M and Asai, S and Aslanides, E and Aßmann, RW and Astapovych, D and Atanasov, M and Atieh, S and Attié, D and Auchmann,
             B and Audurier, A and Aull, S and Aumon, S and Aune, S and Avino, F and Avrillaud, G and Aydın, G and Azatov, A and Azuelos, G and Azzi, P and Azzolini, O and Azzurri, P and Bacchetta, N and Bacchiocchi, E and Bachacou, H and Baek, YW and Baglin, V and Bai, Y and Baird, S and Baker,
             MJ and Baldwin, MJ and Ball, AH and Ballarino, A and Banerjee, S and Barber, DP and Barducci, D and Barjhoux, P},
   Title = {FCC Physics Opportunities: Future Circular Collider
             Conceptual Design Report Volume 1},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {6},
   Year = {2019},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-6904-3},
   Abstract = {We review the physics opportunities of the Future Circular
             Collider, covering its e+e-, pp, ep and heavy ion
             programmes. We describe the measurement capabilities of each
             FCC component, addressing the study of electroweak, Higgs
             and strong interactions, the top quark and flavour, as well
             as phenomena beyond the Standard Model. We highlight the
             synergy and complementarity of the different colliders,
             which will contribute to a uniquely coherent and ambitious
             research programme, providing an unmatchable combination of
             precision and sensitivity to new physics.},
   Doi = {10.1140/epjc/s10052-019-6904-3},
   Key = {fds356591}
}

@article{fds356593,
   Author = {Abada, A and Abbrescia, M and AbdusSalam, SS and Abdyukhanov, I and Abelleira Fernandez and J and Abramov, A and Aburaia, M and Acar, AO and Adzic, PR and Agrawal, P and Aguilar-Saavedra, JA and Aguilera-Verdugo, JJ and Aiba, M and Aichinger, I and Aielli, G and Akay, A and Akhundov, A and Aksakal, H and Albacete, JL and Albergo, S and Alekou, A and Aleksa, M and Aleksan, R and Alemany Fernandez and RM and Alexahin, Y and Alía, RG and Alioli, S and Alipour Tehrani and N and Allanach, BC and Allport, PP and Altınlı, M and Altmannshofer, W and Ambrosio, G and Amorim, D and Amstutz, O and Anderlini, L and Andreazza,
             A and Andreini, M and Andriatis, A and Andris, C and Andronic, A and Angelucci, M and Antinori, F and Antipov, SA and Antonelli, M and Antonello, M and Antonioli, P and Antusch, S and Anulli, F and Apolinário, L and Apollinari, G and Apollonio, A and Appelö, D and Appleby, RB and Apyan, A and Arbey, A and Arbuzov, A and Arduini, G and Arı, V and Arias, S and Armesto, N and Arnaldi, R and Arsenyev, SA and Arzeo, M and Asai, S and Aslanides, E and Aßmann, RW and Astapovych, D and Atanasov, M and Atieh, S and Attié, D and Auchmann, B and Audurier, A and Aull, S and Aumon, S and Aune, S and Avino, F and Avrillaud, G and Aydın,
             G and Azatov, A and Azuelos, G and Azzi, P and Azzolini, O and Azzurri, P and Bacchetta, N and Bacchiocchi, E and Bachacou, H and Baek, YW and Baglin,
             V and Bai, Y and Baird, S and Baker, MJ and Baldwin, MJ and Ball, AH and Ballarino, A and Banerjee, S and Barber, DP and Barducci, D and Barjhoux, P},
   Title = {FCC-ee: The Lepton Collider: Future Circular Collider
             Conceptual Design Report Volume 2},
   Journal = {European Physical Journal: Special Topics},
   Volume = {228},
   Number = {2},
   Pages = {261-623},
   Year = {2019},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjst/e2019-900045-4},
   Abstract = {In response to the 2013 Update of the European Strategy for
             Particle Physics, the Future Circular Collider (FCC) study
             was launched, as an international collaboration hosted by
             CERN. This study covers a highest-luminosity high-energy
             lepton collider (FCC-ee) and an energy-frontier hadron
             collider (FCC-hh), which could, successively, be installed
             in the same 100 km tunnel. The scientific capabilities of
             the integrated FCC programme would serve the worldwide
             community throughout the 21st century. The FCC study also
             investigates an LHC energy upgrade, using FCC-hh technology.
             This document constitutes the second volume of the FCC
             Conceptual Design Report, devoted to the electron-positron
             collider FCC-ee. After summarizing the physics discovery
             opportunities, it presents the accelerator design,
             performance reach, a staged operation scenario, the
             underlying technologies, civil engineering, technical
             infrastructure, and an implementation plan. FCC-ee can be
             built with today’s technology. Most of the FCC-ee
             infrastructure could be reused for FCC-hh. Combining
             concepts from past and present lepton colliders and adding a
             few novel elements, the FCC-ee design promises outstandingly
             high luminosity. This will make the FCC-ee a unique
             precision instrument to study the heaviest known particles
             (Z, W and H bosons and the top quark), offering great direct
             and indirect sensitivity to new physics.},
   Doi = {10.1140/epjst/e2019-900045-4},
   Key = {fds356593}
}

@article{fds356587,
   Author = {Abada, A and Abbrescia, M and AbdusSalam, SS and Abdyukhanov, I and Abelleira Fernandez and J and Abramov, A and Aburaia, M and Acar, AO and Adzic, PR and Agrawal, P and Aguilar-Saavedra, JA and Aguilera-Verdugo, JJ and Aiba, M and Aichinger, I and Aielli, G and Akay, A and Akhundov, A and Aksakal, H and Albacete, JL and Albergo, S and Alekou, A and Aleksa, M and Aleksan, R and Alemany Fernandez and RM and Alexahin, Y and Alía, RG and Alioli, S and Alipour Tehrani and N and Allanach, BC and Allport, PP and Altınlı, M and Altmannshofer, W and Ambrosio, G and Amorim, D and Amstutz, O and Anderlini, L and Andreazza,
             A and Andreini, M and Andriatis, A and Andris, C and Andronic, A and Angelucci, M and Antinori, F and Antipov, SA and Antonelli, M and Antonello, M and Antonioli, P and Antusch, S and Anulli, F and Apolinário, L and Apollinari, G and Apollonio, A and Appelö, D and Appleby, RB and Apyan, A and Arbey, A and Arbuzov, A and Arduini, G and Arı, V and Arias, S and Armesto, N and Arnaldi, R and Arsenyev, SA and Arzeo, M and Asai, S and Aslanides, E and Aßmann, RW and Astapovych, D and Atanasov, M and Atieh, S and Attié, D and Auchmann, B and Audurier, A and Aull, S and Aumon, S and Aune, S and Avino, F and Avrillaud, G and Aydın,
             G and Azatov, A and Azuelos, G and Azzi, P and Azzolini, O and Azzurri, P and Bacchetta, N and Bacchiocchi, E and Bachacou, H and Baek, YW and Baglin,
             V and Bai, Y and Baird, S and Baker, MJ and Baldwin, MJ and Ball, AH and Ballarino, A and Banerjee, S and Barber, DP and Barducci, D and Barjhoux, P},
   Title = {FCC-hh: The Hadron Collider: Future Circular Collider
             Conceptual Design Report Volume 3},
   Journal = {European Physical Journal: Special Topics},
   Volume = {228},
   Number = {4},
   Pages = {755-1107},
   Year = {2019},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjst/e2019-900087-0},
   Abstract = {In response to the 2013 Update of the European Strategy for
             Particle Physics (EPPSU), the Future Circular Collider (FCC)
             study was launched as a world-wide international
             collaboration hosted by CERN. The FCC study covered an
             energy-frontier hadron collider (FCC-hh), a
             highest-luminosity high-energy lepton collider (FCC-ee), the
             corresponding 100 km tunnel infrastructure, as well as the
             physics opportunities of these two colliders, and a
             high-energy LHC, based on FCC-hh technology. This document
             constitutes the third volume of the FCC Conceptual Design
             Report, devoted to the hadron collider FCC-hh. It summarizes
             the FCC-hh physics discovery opportunities, presents the
             FCC-hh accelerator design, performance reach, and staged
             operation plan, discusses the underlying technologies, the
             civil engineering and technical infrastructure, and also
             sketches a possible implementation. Combining ingredients
             from the Large Hadron Collider (LHC), the high-luminosity
             LHC upgrade and adding novel technologies and approaches,
             the FCC-hh design aims at significantly extending the energy
             frontier to 100 TeV. Its unprecedented centre of-mass
             collision energy will make the FCC-hh a unique instrument to
             explore physics beyond the Standard Model, offering great
             direct sensitivity to new physics and discoveries.},
   Doi = {10.1140/epjst/e2019-900087-0},
   Key = {fds356587}
}

@article{fds356710,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Femtoscopy with identified charged pions in proton-lead
             collisions at √sNN =5.02 TeV with ATLAS},
   Journal = {Physical Review C},
   Volume = {96},
   Number = {6},
   Year = {2017},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevC.96.064908},
   Abstract = {Bose-Einstein correlations between identified charged pions
             are measured for p+Pb collisions at sNN=5.02TeV using data
             recorded by the ATLAS detector at the CERN Large Hadron
             Collider corresponding to a total integrated luminosity of
             28nb-1. Pions are identified using ionization energy loss
             measured in the pixel detector. Two-particle correlation
             functions and the extracted source radii are presented as a
             function of collision centrality as well as the average
             transverse momentum (kT) and rapidity (yππ) of the pair.
             Pairs are selected with a rapidity -2<yππ<1 and with an
             average transverse momentum 0.1<kT<0.8GeV. The effect of jet
             fragmentation on the two-particle correlation function is
             studied, and a method using opposite-charge pair data to
             constrain its contributions to the measured correlations is
             described. The measured source sizes are substantially
             larger in more central collisions and are observed to
             decrease with increasing pair kT. A correlation of the radii
             with the local charged-particle density is demonstrated. The
             scaling of the extracted radii with the mean number of
             participating nucleons is also used to compare a selection
             of initial-geometry models. The cross term Rol is measured
             as a function of rapidity, and a nonzero value is observed
             with 5.1σ combined significance for -1<yππ<1 in the most
             central events.},
   Doi = {10.1103/PhysRevC.96.064908},
   Key = {fds356710}
}

@article{fds310383,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H},
   Title = {Fiducial and differential cross sections of Higgs boson
             production measured in the four-lepton decay channel in pp
             collisions at √s=8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {738},
   Pages = {234-253},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.09.054},
   Abstract = {Measurements of fiducial and differential cross sections of
             Higgs boson production in the H→ZZ*→4ℓ decay channel
             are presented. The cross sections are determined within a
             fiducial phase space and corrected for detection efficiency
             and resolution effects. They are based on 20.3fb-1 of pp
             collision data, produced at √s=8 TeV centre-of-mass energy
             at the LHC and recorded by the ATLAS detector. The
             differential measurements are performed in bins of
             transverse momentum and rapidity of the four-lepton system,
             the invariant mass of the subleading lepton pair and the
             decay angle of the leading lepton pair with respect to the
             beam line in the four-lepton rest frame, as well as the
             number of jets and the transverse momentum of the leading
             jet. The measured cross sections are compared to selected
             theoretical calculations of the Standard Model expectations.
             No significant deviation from any of the tested predictions
             is found.},
   Doi = {10.1016/j.physletb.2014.09.054},
   Key = {fds310383}
}

@article{fds347510,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
             H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
             D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
             A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis,
             S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram,
             IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
             Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas,
             CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng,
             Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin,
             V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou,
             Y},
   Title = {Fiducial, total and differential cross-section measurements
             of t-channel single top-quark production in pp
             collisions at 8 TeV using data collected by the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {8},
   Pages = {531},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5061-9},
   Abstract = {Detailed measurements of <i>t</i>-channel single top-quark
             production are presented. They use 20.2 fb[Formula: see
             text] of data collected by the ATLAS experiment in
             proton-proton collisions at a centre-of-mass energy of
             8 TeV at the LHC. Total, fiducial and differential
             cross-sections are measured for both top-quark and
             top-antiquark production. The fiducial cross-section is
             measured with a precision of 5.8% (top quark) and 7.8% (top
             antiquark), respectively. The total cross-sections are
             measured to be [Formula: see text] for top-quark production
             and [Formula: see text] for top-antiquark production, in
             agreement with the Standard Model prediction. In addition,
             the ratio of top-quark to top-antiquark production
             cross-sections is determined to be [Formula: see text]. The
             differential cross-sections as a function of the transverse
             momentum and rapidity of both the top quark and the top
             antiquark are measured at both the parton and particle
             levels. The transverse momentum and rapidity differential
             cross-sections of the accompanying jet from the
             <i>t</i>-channel scattering are measured at particle level.
             All measurements are compared to various Monte Carlo
             predictions as well as to fixed-order QCD calculations where
             available.},
   Doi = {10.1140/epjc/s10052-017-5061-9},
   Key = {fds347510}
}

@article{fds307845,
   Author = {Aaltonen, and T, and al, E},
   Title = {First Measurement of the Angular Coefficients of {Drell-Yan}
             ${e}^{+}{e}^{-}$ Pairs in the ${Z}$ Mass Region from
             $p\overline{p}$ Collisions at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {24},
   Pages = {241801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.241801},
   Abstract = {We report on the first measurement of the angular
             distributions of final state electrons in pp¯ → γ*/Z →
             e(+)e(-) + X events produced in the Z boson mass region at
             √s1.96 TeV. The data sample collected by the CDF II
             detector for this result corresponds to 2.1  fb(-1) of
             integrated luminosity. The angular distributions are studied
             as a function of the transverse momentum of the
             electron-positron pair and show good agreement with the
             Lam-Tung relation, consistent with a spin-1 description of
             the gluon, and demonstrate that, at high values of the
             transverse momentum, Z bosons are produced via
             quark-antiquark annihilation and quark-gluon Compton
             processes.},
   Doi = {10.1103/PhysRevLett.106.241801},
   Key = {fds307845}
}

@article{fds307906,
   Author = {Aaltonen, and T, and others},
   Title = {First Measurement of the b-jet Cross Section in Events with
             a $W$ Boson in $p \bar{p}$ Collisions at $\sqrt{s} = 1.96$
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {13},
   Pages = {131801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.131801},
   Abstract = {http://arxiv.org/abs/0909.1505},
   Doi = {10.1103/PhysRevLett.104.131801},
   Key = {fds307906}
}

@article{fds310269,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {First measurement of the forward-backward asymmetry in
             bottom-quark pair production at high mass},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.032006},
   Abstract = {We measure the particle-level forward-backward production
             asymmetry in bb¯ pairs with masses (mbb¯) larger than 150
             GeV/c2, using events with hadronic jets and employing jet
             charge to distinguish b from b¯. The measurement uses 9.5
             fb-1 of pp¯ collisions at a center-of-mass energy of 1.96
             TeV recorded by the CDF II detector. The asymmetry as a
             function of mbb¯ is consistent with zero, as well as with
             the predictions of the standard model. The measurement
             disfavors a simple model including an axigluon with a mass
             of 200 GeV/c2, whereas a model containing a heavier 345
             GeV/c2 axigluon is not excluded.},
   Doi = {10.1103/PhysRevD.92.032006},
   Key = {fds310269}
}

@article{fds308039,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
             T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
             F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
   Title = {First measurement of the fraction of top-quark pair
             production through gluon-gluon fusion},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {78},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.111101},
   Abstract = {We present the first measurement of σ(gg→tt̄)/
             σ(pp̄→tt̄). We use 0.96fb-1 of s=1.96TeV pp̄ collision
             data recorded with the CDF II detector at Fermilab. Using
             charged particles with low transverse momentum in tt̄
             events, we find σ(gg→ tt̄)/σ(pp̄→tt̄)=0.07±0.14(stat)±0.
             07(syst), corresponding to a 95% confidence level upper
             limit of 0.33, in agreement with the standard model
             next-to-leading-order prediction of 0.15±0.05. © 2008 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.78.111101},
   Key = {fds308039}
}

@article{fds307901,
   Author = {Aaltonen, and T, and others},
   Title = {First Measurement of the Ratio $\sigma_{(t\bar{t})} /
             \sigma_{(Z/\gamma^*\to ll)}$ and Precise Extraction of the
             $t\bar{t}$ Cross Section},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {1},
   Pages = {012001},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.012001},
   Abstract = {http://arxiv.org/abs/1004.3224},
   Doi = {10.1103/PhysRevLett.105.012001},
   Key = {fds307901}
}

@article{fds307971,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart,
             D and Datta, M and Davies, T and Barbaro, PD and Cecco, SD and Deisher, A and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza,
             BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini,
             J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
             C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin,
             M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
             M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
             C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, BY and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
             RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes,
             RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo,
             KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin,
             PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko,
             S and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen,
             AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer,
             MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Griso, SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino,
             G and Pianori, E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
             J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt,
             MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider,
             FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas,
             J},
   Title = {First measurement of the ratio of branching fractions B(Λb
             0→Λc+μ-ν̄μ)/B(Λb 0→Λc+π-)},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.032001},
   Abstract = {This article presents the first measurement of the ratio of
             branching fractions B(Λb0→Λc+μ-ν̄μ)/
             B(Λb0→Λc+π-). Measurements in two control samples using
             the same technique B(B̄0→D+μ- ν̄μ)/B(B̄0→D+π-)
             and B(B̄ 0→D*(2010)+μ-ν̄μ)/ B(B̄0→D*(2010)+π-)
             are also reported. The analysis uses data from an integrated
             luminosity of approximately 172pb-1 of pp̄ collisions at
             s=1.96TeV, collected with the CDF II detector at the
             Fermilab Tevatron. The relative branching fractions are
             measured to be B(Λb 0→Λc+μ-ν̄μ)B(Λb
             0→Λc+π-)=16.6±3.0(stat) ±1.0(syst)+2.6-3.4(PDG)
             ±0.3(EBR), B(B̄0→D+μ-ν̄μ) B(B̄0→D+π-)=9.9±1.0(stat)
             ±0.6(syst)±0.4(PDG)± 0.5(EBR), and B(B̄0→D*(
             2010)+μ-ν̄μ)B(B̄0→D*( 2010)+π-)=16.5±2.3(stat)
             ±0.6(syst)±0.5(PDG)± 0.8(EBR). The uncertainties are from
             statistics (stat), internal systematics (syst), world
             averages of measurements published by the Particle Data
             Group or subsidiary measurements in this analysis (PDG), and
             unmeasured branching fractions estimated from theory (EBR),
             respectively. This article also presents measurements of the
             branching fractions of four new Λb 0 semileptonic decays:
             Λb0→Λc( 2595)+μ-ν̄μ, Λb0→Λc( 2625)+μ-ν̄μ,
             Λb0→Σc( 2455)0π+μ-ν̄μ, and Λb 0→Σc(2455)++π-μ-ν̄μ,
             relative to the branching fraction of the Λb0→Λc+μ-
             ν̄μ decay. Finally, the transverse-momentum distribution
             of Λb0 baryons produced in pp̄ collisions is measured and
             found to be significantly different from that of B̄0
             mesons, which results in a modification in the production
             cross-section ratio σΛb0/σB̄0 with respect to the CDF I
             measurement. © 2009 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.79.032001},
   Key = {fds307971}
}

@article{fds308055,
   Author = {Abulencia, and A, and others},
   Title = {First Measurement of the Ratio of Central-Electron to
             Forward-Electron W Partial Cross Sections in p-pbar
             Collisions at sqrt{s} = 1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {25},
   Pages = {251801},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.251801},
   Abstract = {We present a measurement of sigma(p[overline
             p]-->W){\AA}~[script B](W-->enu) at sqrt(s)=1.96 TeV, using
             electrons identified in the forward region
             (1.2-90+95(syst)$\pm$162(lum) pb. Combining this result with
             a previous CDF measurement obtained using electrons in the
             central region (|eta|},
   Doi = {10.1103/physrevlett.98.251801},
   Key = {fds308055}
}

@article{fds361222,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and González, BÁ and Amerio,
             S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart,
             D and Datta, M and Davies, T and Barbaro, PD and Cecco, SD and Deisher, A and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza,
             BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini,
             J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
             C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin,
             M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
             M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
             C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, BY and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
             RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes,
             RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll,
             J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev,
             DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens,
             P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
             A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao,
             T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer,
             MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Osterberg, K and Griso, SP and Palencia,
             E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks,
             B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus,
             C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Rutherford, B and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt,
             M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber,
             I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer,
             B},
   Title = {First measurement of the tt̄ differential cross section
             dσ/dMtt̄ in pp̄ collisions at s=1.96TeV},
   Journal = {Physical Review Letters},
   Volume = {102},
   Number = {22},
   Pages = {222003},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevLett.102.222003},
   Abstract = {We present a measurement of the tt̄ differential cross
             section with respect to the tt̄ invariant mass, dσ/dMtt̄,
             in pp̄ collisions at s=1.96TeV using an integrated
             luminosity of 2.7fb-1 collected by the CDF II experiment.
             The tt̄ invariant mass spectrum is sensitive to a variety
             of exotic particles decaying into tt̄ pairs. The result is
             consistent with the standard model expectation, as modeled
             by PYTHIA with CTEQ5L parton distribution functions. © 2009
             The American Physical Society.},
   Doi = {10.1103/PhysRevLett.102.222003},
   Key = {fds361222}
}

@article{fds308052,
   Author = {Aaltonen, and T, and others},
   Title = {First Measurement of the W Boson Mass in Run II of the
             Tevatron},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {15},
   Pages = {151801},
   Year = {2007},
   url = {http://link.aps.org/abstract/PRL/v99/e151801},
   Keywords = {W • boson • mass},
   Abstract = {We present a measurement of the W-boson mass using 200 pb-1
             of data collected in p[overline p] collisions at
             sqrt(s)=1.96 TeV by the CDF II detector at run II of the
             Fermilab Tevatron. With a sample of 63 964 W-->enu
             candidates and 51 128 W-->µnu candidates, we measure MW=80
             413$\pm$34stat$\pm$34syst=80 413$\pm$48 MeV/c2. This is the
             most precise single measurement of the W-boson mass to
             date.},
   Doi = {10.1103/physrevlett.99.151801},
   Key = {fds308052}
}

@article{fds327184,
   Author = {Hays, C and Jayatilaka, B and Kotwal, A and Nodulman, L and Stelzer-Chilton, O and Trischuk, W and Vollrath,
             I},
   Title = {First Measurement of the W Boson Mass with CDF in Run
             II},
   Journal = {Journal of Physics: Conference Series},
   Volume = {110},
   Number = {2},
   Pages = {022019-022019},
   Publisher = {IOP Publishing},
   Year = {2008},
   Month = {June},
   url = {http://dx.doi.org/10.1088/1742-6596/110/2/022019},
   Doi = {10.1088/1742-6596/110/2/022019},
   Key = {fds327184}
}

@article{fds308019,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
             T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
             F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and De
             Lorenzo, G and Dell'Orso, M and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di
             Ruzza, B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
             C and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt,
             J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
             S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson,
             W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Koay, SA and Kondo,
             K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus,
             J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
             C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci,
             C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak,
             R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Mangano, ML and Manousakis, A and Margaroli, F and Marino,
             C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
             M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagan Griso,
             S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic,
             V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
             L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó,
             O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro,
             A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
             AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima,
             M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A},
   Title = {First measurement of W boson production in association with
             a single Charm quark in pp collisions at sqrt(s)=1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {100},
   Number = {9},
   Pages = {091803},
   Year = {2008},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.100.091803},
   Abstract = {We present the first measurement of the production cross
             section of a W boson with a single charm quark (c) in pp
             collisions at sqrt(s)=1.96 TeV, using soft muon tagging of c
             jets. In a data sample of approximately 1.8 fb(-1), recorded
             with the Collider Detector at Fermilab II detector at the
             Fermilab Tevatron, we select events with W+1 or 2 jets. We
             use the charge correlation between the W and the muon from
             the semileptonic decay of a charm hadron to extract the Wc
             signal. We measure sigma Wc(PTc >20 GeV/c,|eta c|<1.5) x
             BR(W-->l nu)=9.8+/-3.2 pb, in agreement with theoretical
             expectations.},
   Doi = {10.1103/physrevlett.100.091803},
   Key = {fds308019}
}

@article{fds308135,
   Author = {Acosta, and D, and others},
   Title = {First measurements of inclusive W and Z cross sections from
             Run II of the Tevatron collider},
   Journal = {Phys. Rev. Lett.},
   Volume = {94},
   Number = {9},
   Pages = {091803},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/physrevlett.94.091803},
   Abstract = {http://arxiv.org/abs/hep-ex/0406078},
   Doi = {10.1103/physrevlett.94.091803},
   Key = {fds308135}
}

@article{fds307938,
   Author = {Aaltonen, T and others},
   Title = {First Observation of B̅ s0→Ds ± K∓ and
             Measurement of the Ratio of Branching Fractions B(B̅
             s0→Ds ± K∓)/B(B̅ s0→Ds+π-)},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {19},
   Pages = {191802},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.191802},
   Abstract = {A combined mass and particle identification fit is used to
             make the first observation of the decay B̅ s0→Ds &plusmn;
             K∓ and measure the branching fraction of B̅ s0→Ds
             &plusmn; K∓ relative to B̅ s0→Ds+π-. This analysis
             uses 1.2  fb-1 integrated luminosity of pp̅ collisions
             at sqrt[s]=1.96  TeV collected with the CDF II detector
             at the Fermilab Tevatron collider. We observe a B̅ s0→Ds
             &plusmn; K∓ signal with a statistical significance of
             8.1σ and measure B(B̅ s0→Ds &plusmn; K∓)/B(B̅
             s0→Ds+π-)=0.097 &plusmn; 0.018(stat) &plusmn;
             0.009(syst).},
   Doi = {10.1103/physrevlett.103.191802},
   Key = {fds307938}
}

@article{fds307944,
   Author = {Aaltonen, T and others},
   Title = {First Observation of Vector Boson Pairs in a Hadronic Final
             State at the Tevatron Collider},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {9},
   Pages = {091803},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.091803},
   Abstract = {We present the first observation in hadronic collisions of
             the electroweak production of vector boson pairs (VV, V=W,
             Z) where one boson decays to a dijet final state. The data
             correspond to 3.5  fb-1 of integrated luminosity of pp̅
             collisions at sqrt[s]=1.96  TeV collected by the CDF II
             detector at the Fermilab Tevatron. We observe 1516 &plusmn;
             239(stat) &plusmn; 144(syst) diboson candidate events and
             measure a cross section σ(pp̅ →VV+X) of 18.0 &plusmn;
             2.8(stat) &plusmn; 2.4(syst) &plusmn; 1.1(lumi)  pb, in
             agreement with the expectations of the standard
             model.},
   Doi = {10.1103/physrevlett.103.091803},
   Key = {fds307944}
}

@article{fds308027,
   Author = {Kotwal, AV and Collaboration, TCDF},
   Title = {First Run II Measurement of the W boson Mass},
   Journal = {Physical Review D},
   Volume = {77},
   Number = {112001},
   Pages = {48},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.112001},
   Abstract = {We describe a measurement of the W boson mass mW using
             200pb-1 of s=1.96TeV pp̄ collision data taken with the CDF
             II detector. With a sample of 63964 W→eν candidates and
             51128 W→μν candidates, we measure mW=[80.413±0.034(stat)±0.034(sys)=80.413±0.048]GeV/c2.
             This is the single most precise mW measurement to date. When
             combined with other measured electroweak parameters, this
             result further constrains the properties of new unobserved
             particles coupling to W and Z bosons. © 2008 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.77.112001},
   Key = {fds308027}
}

@article{fds307549,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
             JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
             A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
             C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
             L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester Iii and WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {First search for exotic Z Boson decays into photons and
             neutral pions in hadron collisions.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {11},
   Pages = {111803},
   Year = {2014},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.112.111803},
   Abstract = {A search for forbidden and exotic Z boson decays in the
             diphoton mass spectrum is presented for the first time in
             hadron collisions, based on data corresponding to 10.0
             fb(-1) of integrated luminosity from proton-antiproton
             collisions at √s = 1.96 TeV collected by the CDF
             experiment. No evidence of signal is observed, and 95%
             credibility level Bayesian upper limits are set on the
             branching ratios of decays of the Z boson to a photon and
             neutral pion (which is detected as a photon), a pair of
             photons, and a pair of neutral pions. The observed branching
             ratio limits are 2.01 × 10(-5) for Z → π(0)γ, 1.46 ×
             10(-5) for Z → γγ, and 1.52 × 10(-5) for Z →
             π(0)π(0). The Z → π(0)γ and Z → γγ limits improve
             the most stringent results from other experiments by factors
             of 2.6 and 3.6, respectively. The Z → π(0)π(0) branching
             ratio limit is the first experimental result on this
             decay.},
   Doi = {10.1103/physrevlett.112.111803},
   Key = {fds307549}
}

@article{fds307843,
   Author = {Aaltonen, and T, and al, E},
   Title = {First Search for Multijet Resonances in $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$
             $p\overline{p}$ Collisions},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {4},
   Pages = {042001},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.042001},
   Abstract = {We present the first model independent search for three-jet
             hadronic resonances within multijet events in sqrt(s) =
             1.96  TeV pp collisions at the Fermilab Tevatron using
             the CDF II detector. Pair production of supersymmetric
             gluinos and squarks with hadronic R-parity violating decays
             is employed as an example of a new physics benchmark for
             this signature. Selection criteria based on the kinematic
             properties of an ensemble of jet combinations within each
             event help to extract signal from copious QCD background. No
             significant excess outside the top quark mass window is
             observed in data with an integrated luminosity of
             3.2  fb(-1). We place 95% confidence level limits on the
             production cross section σ(pp → XX')×BR(gg →
             3  jet + 3  jet) where X, X' = g, q, or q, with q, q
             → g + jet, as a function of gluino mass, in the range of
             77  GeV/c2 to 240  GeV/c2.},
   Doi = {10.1103/PhysRevLett.107.042001},
   Key = {fds307843}
}

@article{fds307974,
   Author = {Aaltonen, T and others},
   Title = {First simultaneous measurement of the top quark mass in the
             lepton + jets and dilepton channels at CDF},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {9},
   Pages = {092005},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.092005},
   Abstract = {We present a measurement of the mass of the top quark using
             data corresponding to an integrated luminosity of 1.9fb-1 of
             pp̄ collisions collected at s=1.96TeV with the CDF II
             detector at Fermilab's Tevatron. This is the first
             measurement of the top quark mass using top-antitop pair
             candidate events in the lepton+jets and dilepton decay
             channels simultaneously. We reconstruct two observables in
             each channel and use a nonparametric kernel density
             estimation technique to derive two-dimensional probability
             density functions from simulated signal and background
             samples. The observables are the top quark mass and the
             invariant mass of two jets from the W decay in the
             lepton+jets channel, and the top quark mass and the scalar
             sum of transverse energy of the event in the dilepton
             channel. We perform a simultaneous fit for the top quark
             mass and the jet energy scale, which is constrained in situ
             by the hadronic W boson mass. Using 332 lepton+jets
             candidate events and 144 dilepton candidate events, we
             measure the top quark mass to be Mtop=171.9±1.
             7(stat+JES)±1.1(othersyst)GeV/c2=171.9±2.0GeV/c2. © 2009
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.79.092005},
   Key = {fds307974}
}

@article{fds310359,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ},
   Title = {Flavor tagged time-dependent angular analysis of the Bs0
             →J/ψφ decay and extraction of ΔΓs and the weak phase
             φs in ATLAS},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.052007},
   Abstract = {A measurement of the Bs0→J/ψφ decay parameters, updated
             to include flavor tagging is reported using 4.9fb-1 of
             integrated luminosity collected by the ATLAS detector from
             s=7TeV pp collisions recorded in 2011 at the LHC. The values
             measured for the physical parameters are
             φs=0.12±0.25(stat)±0.05(syst)radΔΓs=0.053±0.021(stat)±0.010(syst)ps-1Γs=0.677±0.007(stat)±0.004(syst)ps-1|A
             (0)|2=0.220±0.008(stat)±0.009(syst)|A0(0)|2=0.529±0.006(stat)±0.012(syst)δ=3.89±0.47(stat)±0.11(syst)radwhere
             the parameter ΔΓs is constrained to be positive. The
             S-wave contribution was measured and found to be compatible
             with zero. Results for φs and ΔΓs are also presented as
             68% and 95% likelihood contours, which show agreement with
             the Standard Model expectations.},
   Doi = {10.1103/PhysRevD.90.052007},
   Key = {fds310359}
}

@article{fds347521,
   Author = {Kakati, B and Kotwal, A and Biswas, D and Sahu, S},
   Title = {Fluconazole Resistant Candida Oesophagitis in
             Immunocompetent Patients: Is Empirical Therapy
             Justifiable?},
   Journal = {Journal of clinical and diagnostic research :
             JCDR},
   Volume = {9},
   Number = {12},
   Pages = {DC16-DC18},
   Year = {2015},
   Month = {December},
   url = {http://dx.doi.org/10.7860/jcdr/2015/15171.6975},
   Abstract = {<h4>Introduction</h4>C. albicans (Candida albicans) is the
             foremost cause of fungal oesophagitis, however other species
             such as Candida tropicalis, Candida krusei and Candida
             stellatoidea have also been implicated to cause this
             condition. Although, numerous studies have identified risk
             factors for C. albicans oesophagitis, data for non- C.
             albicans species is still sparse.<h4>Aim</h4>To determine
             the aetiology of Candida oesophagitis in our medical centre
             over a two year period. Additionally, to investigate
             predisposing conditions for oesophageal candidiasis caused
             by different Candida species.<h4>Material and
             methods</h4>All consecutive patients posted for upper
             gastrointestinal endoscopy at the endoscopy unit of a
             tertiary care hospital in north India with findings
             consistent with oesophagitis were screened for the presence
             of Candida oesophagitis by performing KOH (potassium
             hydroxide) examination and culture on SDA (Sabouraud's
             dextrose agar). Antifungal susceptibility testing as per
             CLSI guidelines was performed for fluconazole, a most common
             empirically prescribed antifungal for the
             condition.<h4>Results</h4>A total of 1868 patients with no
             known immune-compromised condition underwent upper
             gastroscopy at our centre during the study period. The
             prevalence of Candida oesophagitis was 8.7% (n = 163). C.
             albicans was recovered from majority of infections (52.1%),
             followed by C. tropicalis (24%), C. parapsilosis (13.4%), C.
             glabrata (6.9%) and C. krusei (3.6%). Alarmingly, among the
             C. albicans isolates 8.6% were resistant to
             fluconazole.<h4>Conclusion</h4>With rising reports of
             antifungal drug resistance among the isolates of Candida
             species, an increasing prevalence of this organism could
             have an impact on the treatment of Candidal oesophagitis and
             it should be approached with caution by the
             clinician.},
   Doi = {10.7860/jcdr/2015/15171.6975},
   Key = {fds347521}
}

@article{fds356548,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
             Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
             NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
             J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP},
   Title = {Fluctuations of anisotropic flow in Pb+Pb collisions at
             √sNN = 5.02 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {1},
   Year = {2020},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2020)051},
   Abstract = {Multi-particle azimuthal cumulants are measured as a
             function of centrality and transverse momentum using 470
             μb−1 of Pb+Pb collisions at sNN = 5.02 TeV with the ATLAS
             detector at the LHC. These cumulants provide information on
             the event-by-event fluctuations of harmonic flow
             coefficients vn and correlated fluctuations between two
             harmonics vn and vm. For the first time, a non-zero
             four-particle cumulant is observed for dipolar flow, v1. The
             four-particle cumulants for elliptic flow, v2, and
             triangular flow, v3, exhibit a strong centrality dependence
             and change sign in ultra-central collisions. This sign
             change is consistent with significant non-Gaussian
             fluctuations in v2 and v3. The four-particle cumulant for
             quadrangular flow, v4, is found to change sign in
             mid-central collisions. Correlations between two harmonics
             are studied with three- and four-particle mixed-harmonic
             cumulants, which indicate an anti-correlation between v2 and
             v3, and a positive correlation between v2 and v4. These
             correlations decrease in strength towards central collisions
             and either approach zero or change sign in ultra-central
             collisions. To investigate the possible flow fluctuations
             arising from intrinsic centrality or volume fluctuations,
             the results are compared between two different event classes
             used for centrality definitions. In peripheral and
             mid-central collisions where the cumulant signals are large,
             only small differences are observed. In ultra-central
             collisions, the differences are much larger and transverse
             momentum dependent. These results provide new information to
             disentangle flow fluctuations from the initial and final
             states, as well as new insights on the influence of
             centrality fluctuations. [Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP01(2020)051},
   Key = {fds356548}
}

@article{fds312244,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Forward-backward correlations and charged-particle azimuthal
             distributions in pp interactions using the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {7},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP07(2012)019},
   Abstract = {Using inelastic proton-proton interactions at √s =900 GeV
             and 7TeV, recorded by the ATLAS detector at the LHC,
             measurements have been made of the correlations between
             forward and backward charged-particle multiplicities and,
             for the first time, between forward and backward
             charged-particle summed transverse momentum. In addition,
             jet-like structure in the events is studied by means of
             azimuthal distributions of charged particles relative to the
             charged particle with highest transverse momentum in a
             selected kinematic region of the event. The results are
             compared with predictions from tunes of the PYTHIA and
             HERWIG++ Monte Carlo generators, which in most cases are
             found to provide a reasonable description of the
             data.},
   Doi = {10.1007/JHEP07(2012)019},
   Key = {fds312244}
}

@article{fds307728,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães Da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman De Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Forward-backward correlations and charged-particle azimuthal
             distributions in pp interactions using the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {7},
   Year = {2012},
   url = {http://dx.doi.org/10.1007/JHEP07(1992)019},
   Abstract = {Using inelastic proton-proton interactions at √s =900 GeV
             and 7TeV, recorded by the ATLAS detector at the LHC,
             measurements have been made of the correlations between
             forward and backward charged-particle multiplicities and,
             for the first time, between forward and backward
             charged-particle summed transverse momentum. In addition,
             jet-like structure in the events is studied by means of
             azimuthal distributions of charged particles relative to the
             charged particle with highest transverse momentum in a
             selected kinematic region of the event. The results are
             compared with predictions from tunes of the PYTHIA and
             HERWIG++ Monte Carlo generators, which in most cases are
             found to provide a reasonable description of the
             data.},
   Doi = {10.1007/JHEP07(1992)019},
   Key = {fds307728}
}

@article{fds347538,
   Author = {Patyal, S and Kotwal, A and Banarji, A and Gurunadh,
             VS},
   Title = {Frequency doubling technology and standard automated
             perimetry in detection of glaucoma among glaucoma
             suspects.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {70},
   Number = {4},
   Pages = {332-337},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.mjafi.2013.09.002},
   Abstract = {<h4>Background</h4>Frequency Doubling perimetry (FDT) has
             been found to precede visual loss detected by standard
             automated perimetry (SAP) by as much as four years and the
             initial development of glaucomatous visual field loss as
             measured by SAP was found to occur in regions that had
             previously demonstrated abnormalities on FDT
             testing.<h4>Methods</h4>A study on 55 glaucoma suspects
             (determined as per American Academy Guidelines, Preferred
             Practice Pattern, Oct 2010), was compared to 50 healthy
             participants (HP). Both glaucoma suspects and HP underwent
             SAP and FDT in random order. Only reliable fields were
             compared.<h4>Results</h4>Mean deviation of FDT Matrix was
             significantly lower than SAP SITA in suspect and healthy
             group ; two devices showed significant correlation amongst
             both groups (suspects p = 0.002, healthy p = 0.011).
             Significant difference was found in PSD of SAP SITA and FDT
             Matrix (p = 0.001) in the glaucoma suspect group, PSD of FDT
             Matrix was significantly higher than PSD of SAP SITA in the
             healthy group (p < 0.001). PSD of SAP SITA significantly
             correlated with FDT Matrix PSD in glaucoma group (r = 0.579;
             p = 0.001) but no significant correlation found in healthy
             group (r = 0.153; p = 0.290). Percentages of normal test
             locations significantly higher in FDT Matrix compared to SAP
             SITA in glaucoma suspects and healthy participants.<h4>Conclusion</h4>FDT
             correlates well with SAP and may be used for patients who
             are unable to perform well and reliably with SAP but does
             not show any features of earlier glaucoma changes in this
             study.},
   Doi = {10.1016/j.mjafi.2013.09.002},
   Key = {fds347538}
}

@article{fds307671,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Kesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Further search for supersymmetry at √s=7TeV in final
             states with jets, missing transverse momentum, and isolated
             leptons with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.092002},
   Abstract = {This work presents a new inclusive search for supersymmetry
             (SUSY) by the ATLAS experiment at the LHC in proton-proton
             collisions at a center-of-mass energy √s=7TeV in final
             states with jets, missing transverse momentum and one or
             more isolated electrons and/or muons. The search is based on
             data from the full 2011 data-taking period, corresponding to
             an integrated luminosity of 4.7fb-1. Single-lepton and
             multilepton channels are treated together in one analysis.
             An increase in sensitivity is obtained by simultaneously
             fitting the number of events in statistically independent
             signal regions, and the shapes of distributions within those
             regions. A dedicated signal region is introduced to be
             sensitive to decay cascades of SUSY particles with small
             mass differences ("compressed SUSY"). Background
             uncertainties are constrained by fitting to the
             jet-multiplicity distribution in background control regions.
             Observations are consistent with Standard Model
             expectations, and limits are set or extended on a number of
             SUSY models. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.86.092002},
   Key = {fds307671}
}

@article{fds346192,
   Author = {Agrawal, S and Deo, J and Verma, AK and Kotwal, A},
   Title = {Geriatric health: need to make it an essential element of
             primary health care.},
   Journal = {Indian journal of public health},
   Volume = {55},
   Number = {1},
   Pages = {25-29},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.4103/0019-557x.82540},
   Abstract = {Within the next few decades, we will see an extraordinary
             increase in the number of older people worldwide. The public
             health benefit of preventive medicine in old age comes from
             the compression of the time spent in dependency to a
             minimum. A community-based, cross-sectional study was
             conducted to assess the morbidity profile of the geriatric
             population in a rural area of Maharashtra. A total of 214
             subjects, of age 60 years and above, were examined. Data
             were collected by structured interviews and clinical and
             laboratory examinations. Out of the total of 214 subjects,
             190 were suffering from some or the other diseases and the
             major morbidities were visual (56%), musculoskeletal
             (38.3%), respiratory (32.7%), and hypertension (28%). Anemia
             was present in 62.6%, 5.61% had Diabetes Mellitus and 22.5%
             were found to be overweight. The average morbidity load was
             2.61. The rising morbidities clearly showed that a regular,
             complete health checkup of the elderly should be embedded in
             the essential elements of the Primary Health Care. This
             would reduce the morbidity, improve the quality of life, and
             facilitate 'Active Aging'.},
   Doi = {10.4103/0019-557x.82540},
   Key = {fds346192}
}

@article{fds307976,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Aurisano, A and Azfar, F and Azzurri, P and Badgett,
             W and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
             S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung,
             K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci,
             MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway,
             J},
   Title = {Global search for new physics with 2.0fb-1 at
             CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.011101},
   Abstract = {Data collected in run II of the Fermilab Tevatron are
             searched for indications of new electroweak-scale physics.
             Rather than focusing on particular new physics scenarios,
             CDF data are analyzed for discrepancies with the standard
             model prediction. A model-independent approach (Vista)
             considers gross features of the data, and is sensitive to
             new large cross-section physics. Further sensitivity to new
             physics is provided by two additional algorithms: a Bump
             Hunter searches invariant mass distributions for "bumps"
             that could indicate resonant production of new particles,
             and the Sleuth procedure scans for data excesses at large
             summed transverse momentum. This combined global search for
             new physics in 2.0fb-1 of pp̄ collisions at s=1.96TeV
             reveals no indication of physics beyond the standard model.
             © 2009 The American Physical Society.},
   Doi = {10.1103/PhysRevD.79.011101},
   Key = {fds307976}
}

@article{fds346210,
   Author = {Kotwal, A and Priya, R and Qadeer, I},
   Title = {Goiter and other iodine deficiency disorders: A systematic
             review of epidemiological studies to deconstruct the complex
             web.},
   Journal = {Archives of medical research},
   Volume = {38},
   Number = {1},
   Pages = {1-14},
   Year = {2007},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.arcmed.2006.08.006},
   Abstract = {A systematic review of the available literature on goiter
             and other iodine deficiency disorders (IDDs) was carried out
             with the aim of analyzing available evidence and providing
             inputs to the policy makers and program formulators
             regarding the entire issue. The findings point to major
             issues such as the following: methodological issues in
             epidemiology of goiter and other iodine deficiency disorders
             (IDDs); lacunae in causal linkages; inadequate attention to
             multicausality; flawed assessment of the impact of
             intervention, i.e., iodized salt; and harmful effects of
             iodine not given due cognizance. Most of the research to
             date has been unidirectional and does not provide
             comprehensive data on all aspects of IDDs. To further
             compound the issue, many independent researchers, on finding
             something different from the existing dominant paradigm
             (iodized salt as panacea for goiter) have tended to ignore
             these in their final conclusions and recommendations. Thus,
             evidence from this systematic review demonstrates enough
             basis to start a debate on the entire issue, recognizing
             opposing research findings while continuing with the present
             strategy. This imposes specific problems and necessitates
             area-specific solutions instead of a universal solution,
             which apart from being less effective may be harmful in the
             long run.},
   Doi = {10.1016/j.arcmed.2006.08.006},
   Key = {fds346210}
}

@article{fds346183,
   Author = {Anargh, V and Singh, H and Kulkarni, A and Kotwal, A and Mahen,
             A},
   Title = {Hand hygiene practices among health care workers (HCWs) in a
             tertiary care facility in Pune.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {69},
   Number = {1},
   Pages = {54-56},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.mjafi.2012.08.011},
   Abstract = {<h4>Background</h4>Improper hand hygiene by healthcare
             workers (HCWs) is responsible for about 40% of nosocomial
             infections resulting in prolonged illnesses, hospital stays,
             long-term disability and unexpected high costs on patients
             and their families, and also lead to a massive additional
             financial burden on the health-care system.<h4>Objective</h4>To
             assess knowledge and practices regarding hand hygiene among
             HCWs of a tertiary health care facility.<h4>Methods</h4>A
             cross sectional, questionnaire and observation based study
             was carried out in a tertiary care health care facility in
             Pune. Based on sample size calculations, 100 HCWs working in
             medical and surgical wards were studied.<h4>Results</h4>The
             proportion knowledgeable about hand hygiene practices was
             85% and 73% HCWs were of the belief that unclean hands are
             an important route of cross transmission. WHO guidelines
             regarding procedure were being followed by 90% for hand
             washing with soap and water and 64% for alcohol based rubs.
             Majority preferred hand washing with soap and water over
             hand rubbing with alcohol based solutions. 21% of HCWs were
             missing hand hygiene opportunities 1 in 5 times. Heavy
             workload (38%), non availability (52%) and inaccessibility
             (9%) of hand hygiene facilities were the common reasons for
             non-compliance. Availability of 'one time use paper towels'
             was low (12%).<h4>Conclusion</h4>Inadequate compliance
             despite knowledge and false sense of security by alcohol
             based rubs was seen. A multi disciplinary, multifaceted
             approach is required to tackle issues of
             non-compliance.},
   Doi = {10.1016/j.mjafi.2012.08.011},
   Key = {fds346183}
}

@article{fds331389,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
             VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Bolton,
             TA and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
             F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and De,
             K and De Jong and SJ and Demarteau, M and Demina, R and Demine, P and Denisov,
             D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV and Duensing, S and Duflot,
             L},
   Title = {Hard single diffraction in p̄ p collisions at √s = 630
             and 1800 GeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {531},
   Number = {1-2},
   Pages = {52-60},
   Publisher = {Elsevier BV},
   Year = {2002},
   Month = {April},
   url = {http://dx.doi.org/10.1016/S0370-2693(02)01364-3},
   Abstract = {Using the DØ detector, we have studied events produced in
             p-p collisions that contain large forward regions with very
             little energy deposition ("rapidity gaps") and concurrent
             jet production at center-of-mass energies of √s = 630 and
             1800 GeV. The fraction of events with forward or central
             jets associated with rapidity gaps is compared to
             predictions for hard diffraction. We also extract the
             momentum loss for scattered protons in such
             processes.},
   Doi = {10.1016/S0370-2693(02)01364-3},
   Key = {fds331389}
}

@article{fds346161,
   Author = {Abada, A and Abbrescia, M and AbdusSalam, SS and Abdyukhanov, I and Abelleira Fernandez and J and Abramov, A and Aburaia, M and Acar, AO and Adzic, PR and Agrawal, P and Aguilar-Saavedra, JA and Aguilera-Verdugo, JJ and Aiba, M and Aichinger, I and Aielli, G and Akay, A and Akhundov, A and Aksakal, H and Albacete, JL and Albergo, S and Alekou, A and Aleksa, M and Aleksan, R and Alemany Fernandez and RM and Alexahin, Y and Alía, RG and Alioli, S and Alipour Tehrani and N and Allanach, BC and Allport, PP and Altınlı, M and Altmannshofer, W and Ambrosio, G and Amorim, D and Amstutz, O and Anderlini, L and Andreazza,
             A and Andreini, M and Andriatis, A and Andris, C and Andronic, A and Angelucci, M and Antinori, F and Antipov, SA and Antonelli, M and Antonello, M and Antonioli, P and Antusch, S and Anulli, F and Apolinário, L and Apollinari, G and Apollonio, A and Appelö, D and Appleby, RB and Apyan, A and Arbey, A and Arbuzov, A and Arduini, G and Arı, V and Arias, S and Armesto, N and Arnaldi, R and Arsenyev, SA and Arzeo, M and Asai, S and Aslanides, E and Aßmann, RW and Astapovych, D and Atanasov, M and Atieh, S and Attié, D and Auchmann, B and Audurier, A and Aull, S and Aumon, S and Aune, S and Avino, F and Avrillaud, G and Aydın,
             G and Azatov, A and Azuelos, G and Azzi, P and Azzolini, O and Azzurri, P and Bacchetta, N and Bacchiocchi, E and Bachacou, H and Baek, YW and Baglin,
             V and Bai, Y and Baird, S and Baker, MJ and Baldwin, MJ and Ball, AH and Ballarino, A and Banerjee, S and Barber, DP and Barducci, D and Barjhoux, P},
   Title = {HE-LHC: The High-Energy Large Hadron Collider: Future
             Circular Collider Conceptual Design Report Volume
             4},
   Journal = {European Physical Journal: Special Topics},
   Volume = {228},
   Number = {5},
   Pages = {1109-1382},
   Year = {2019},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjst/e2019-900088-6},
   Abstract = {In response to the 2013 Update of the European Strategy for
             Particle Physics (EPPSU), the Future Circular Collider (FCC)
             study was launched as a world-wide international
             collaboration hosted by CERN. The FCC study covered an
             energy-frontier hadron collider (FCC-hh), a
             highest-luminosity high-energy lepton collider (FCC-ee), the
             corresponding 100 km tunnel infrastructure, as well as the
             physics opportunities of these two colliders, and a
             high-energy LHC, based on FCC-hh technology. This document
             constitutes the third volume of the FCC Conceptual Design
             Report, devoted to the hadron collider FCC-hh. It summarizes
             the FCC-hh physics discovery opportunities, presents the
             FCC-hh accelerator design, performance reach, and staged
             operation plan, discusses the underlying technologies, the
             civil engineering and technical infrastructure, and also
             sketches a possible implementation. Combining ingredients
             from the Large Hadron Collider (LHC), the high-luminosity
             LHC upgrade and adding novel technologies and approaches,
             the FCC-hh design aims at significantly extending the energy
             frontier to 100 TeV. Its unprecedented centre-of-mass
             collision energy will make the FCC-hh a unique instrument to
             explore physics beyond the Standard Model, offering great
             direct sensitivity to new physics and discoveries.},
   Doi = {10.1140/epjst/e2019-900088-6},
   Key = {fds346161}
}

@article{fds346195,
   Author = {Kotwal, A and Taneja, D},
   Title = {Health Care Workers and Universal Precautions: Perceptions
             and Determinants of Non-compliance.},
   Journal = {Indian journal of community medicine : official publication
             of Indian Association of Preventive & Social
             Medicine},
   Volume = {35},
   Number = {4},
   Pages = {526-528},
   Year = {2010},
   Month = {October},
   url = {http://dx.doi.org/10.4103/0970-0218.74373},
   Doi = {10.4103/0970-0218.74373},
   Key = {fds346195}
}

@article{fds352787,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
             MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
             CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA and Arcangeletti,
             C},
   Title = {Higgs boson production cross-section measurements and their
             EFT interpretation in the 4 ℓ decay channel at √s=
             13 TeV with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {10},
   Year = {2020},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-8227-9},
   Abstract = {Higgs boson properties are studied in the four-lepton decay
             channel (where lepton = e, μ) using 139 fb - 1 of
             proton–proton collision data recorded at s=13 TeV by the
             ATLAS experiment at the Large Hadron Collider. The inclusive
             cross-section times branching ratio for H→ ZZ∗ decay is
             measured to be 1.34 ± 0.12 pb for a Higgs boson with
             absolute rapidity below 2.5, in good agreement with the
             Standard Model prediction of 1.33 ± 0.08 pb. Cross-sections
             times branching ratio are measured for the main Higgs boson
             production modes in several exclusive phase-space regions.
             The measurements are interpreted in terms of coupling
             modifiers and of the tensor structure of Higgs boson
             interactions using an effective field theory approach.
             Exclusion limits are set on the CP-even and CP-odd ‘beyond
             the Standard Model’ couplings of the Higgs boson to vector
             bosons, gluons and top quarks.},
   Doi = {10.1140/epjc/s10052-020-8227-9},
   Key = {fds352787}
}

@article{fds307578,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
             T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
             R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
             D and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brucken, E and Budagov, J and Bu, XB and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu,
             A},
   Title = {Higgs boson studies at the Tevatron},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.052014},
   Abstract = {We combine searches by the CDF and D0 Collaborations for the
             standard model Higgs boson with mass in the range 90-200
             GeV/c2 produced in the gluon-gluon fusion, WH, ZH, tt̄H,
             and vector boson fusion processes, and decaying in the
             H→bb̄, H→W+W-, H→ZZ, H→τ+τ-, and H→γγ modes.
             The data correspond to integrated luminosities of up to 10
             fb-1 and were collected at the Fermilab Tevatron in pp̄
             collisions at √s=1.96 TeV. The searches are also
             interpreted in the context of fermiophobic and fourth
             generation models. We observe a significant excess of events
             in the mass range between 115 and 140 GeV/c2. The local
             significance corresponds to 3.0 standard deviations at
             mH=125 GeV/c2, consistent with the mass of the Higgs boson
             observed at the LHC, and we expect a local significance of
             1.9 standard deviations. We separately combine searches for
             H→bb̄, H→W +W-, H→τ+τ-, and H→γγ. The observed
             signal strengths in all channels are consistent with the
             presence of a standard model Higgs boson with a mass of 125
             GeV/c2. © 2013 American Physical Society.},
   Doi = {10.1103/PhysRevD.88.052014},
   Key = {fds307578}
}

@article{fds362575,
   Author = {Dawson, S and Gritsan, A and Logan, H and Qian, J and Tully, C and Kooten,
             RV and Ajaib, A and Anastassov, A and Anderson, I and Asner, D and Bake, O and Barger, V and Barklow, T and Batell, B and Battaglia, M and Berge, S and Blondel, A and Bolognesi, S and Brau, J and Brownson, E and Cahill-Rowley, M and Calancha-Paredes, C and Chen, C-Y and Chou, W and Clare, R and Cline, D and Craig, N and Cranmer, K and Gruttola, MD and Elagin, A and Essig, R and Everett, L and Feng, E and Fujii, K and Gainer,
             J and Gao, Y and Gogoladze, I and Gori, S and Goncalo, R and Graf, N and Grojean, C and Guindon, S and Haber, H and Han, T and Hanson, G and Harnik,
             R and Heinemeyer, S and Heintz, U and Hewett, J and Ilchenko, Y and Ishikawa, A and Ismail, A and Jain, V and Janot, P and Kanemura, S and Kawada, S and Kehoe, R and Klute, M and Kotwal, A and Krueger, K and Kukartsev, G and Kumar, K and Kunkle, J and Kurata, M and Lewis, I and Li,
             Y and Linssen, L and Lipeles, E and Lipton, R and Liss, T and List, J and Liu,
             T and Liu, Z and Low, I and Ma, T and Mackenzie, P and Mellado, B and Melnikov, K and Miyamoto, A and Moortgat-Pick, G and Mourou, G and Narain, M and Neal, H and Nielsen, J and Okada, N and Okawa, H and Olsen,
             J and Ono, H and Onyisi, P and Parashar, N and Peskin, M and Petriello, F and Plehn, T and Pollard, C and Potter, C and Prokofiev, K and Rauch, M and Rizzo, T and Robens, T and Rodriguez, V and Roloff, P and Ruiz, R and Sanz,
             V and Sayre, J and Shafi, Q and Shaughnessy, G and Sher, M and Simon, F and Solyak, N and Strube, J and Stupak, J and Su, S and Suehara, T and Tanabe,
             T and Tajima, T and Telnov, V and Tian, J and Thomas, S and Thomson, M and Tsumura, K and Un, C and Velasco, M and Wagner, C and Wang, S and Watanuki,
             S and Weiglein, G and Whitbeck, A and Yagyu, K and Yao, W and Yokoya, H and Zenz, S and Zerwas, D and Zhang, Y and Zhou, Y},
   Title = {Higgs Working Group Report of the Snowmass 2013 Community
             Planning Study},
   Year = {2013},
   Month = {October},
   Abstract = {This report summarizes the work of the Energy Frontier Higgs
             Boson working group of the 2013 Community Summer Study
             (Snowmass). We identify the key elements of a precision
             Higgs physics program and document the physics potential of
             future experimental facilities as elucidated during the
             Snowmass study. We study Higgs couplings to gauge boson and
             fermion pairs, double Higgs production for the Higgs
             self-coupling, its quantum numbers and $CP$-mixing in Higgs
             couplings, the Higgs mass and total width, and prospects for
             direct searches for additional Higgs bosons in extensions of
             the Standard Model. Our report includes projections of
             measurement capabilities from detailed studies of the
             Compact Linear Collider (CLIC), a Gamma-Gamma Collider, the
             International Linear Collider (ILC), the Large Hadron
             Collider High-Luminosity Upgrade (HL-LHC), Very Large Hadron
             Colliders up to 100 TeV (VLHC), a Muon Collider, and a
             Triple-Large Electron Positron Collider (TLEP).},
   Key = {fds362575}
}

@article{fds346211,
   Author = {Kotwal, J and Apte, CV and Kotwal, A and Mukherjee, B and Jayaram,
             J},
   Title = {High altitude: a hypercoagulable state: results of a
             prospective cohort study.},
   Journal = {Thrombosis research},
   Volume = {120},
   Number = {3},
   Pages = {391-397},
   Year = {2007},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.thromres.2006.09.013},
   Doi = {10.1016/j.thromres.2006.09.013},
   Key = {fds346211}
}

@article{fds356752,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
             H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and AlvarezGonzalez, B and ÁlvarezPiqueras, D and Alviggi, MG and Amadio, BT and AmaralCoutinho, Y and Amelung, C and Amidei, D and AmorDosSantos, SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and AperioBella, L and Arabidze, G and Arai, Y and Araque,
             JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik,
             M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
   Title = {High-ET isolated-photon plus jets production in
             pp collisions at s=8 TeV with the ATLAS detector},
   Journal = {Nuclear Physics B},
   Volume = {918},
   Pages = {257-316},
   Year = {2017},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.nuclphysb.2017.03.006},
   Abstract = {The dynamics of isolated-photon plus one-, two- and
             three-jet production in pp collisions at a centre-of-mass
             energy of 8 TeV are studied with the ATLAS detector at the
             LHC using a data set with an integrated luminosity of 20.2
             fb−1. Measurements of isolated-photon plus jets cross
             sections are presented as functions of the photon and jet
             transverse momenta. The cross sections as functions of the
             azimuthal angle between the photon and the jets, the
             azimuthal angle between the jets, the photon–jet invariant
             mass and the scattering angle in the photon–jet
             centre-of-mass system are presented. The pattern of QCD
             radiation around the photon and the leading jet is
             investigated by measuring jet production in an annular
             region centred on each object; enhancements are observed
             around the leading jet with respect to the photon in the
             directions towards the beams. The experimental measurements
             are compared to several different theoretical calculations,
             and overall a good description of the data is
             found.},
   Doi = {10.1016/j.nuclphysb.2017.03.006},
   Key = {fds356752}
}

@article{fds362779,
   Author = {CDF Collaboration†‡, and Aaltonen, T and Amerio, S and Amidei,
             D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland,
             KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Carls, B and Carlsmith, D and Carosi, R and Carrillo,
             S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes,
             RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori,
             M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
             JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen,
             AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles,
             E and Lister, A and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti,
             P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian,
             C and Miao, T and Michielin, E and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro,
             A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet,
             M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, K and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang, SM and Waters,
             D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfmeister, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli,
             S},
   Title = {High-precision measurement of the W boson mass with
             the CDF II detector.},
   Journal = {Science (New York, N.Y.)},
   Volume = {376},
   Number = {6589},
   Pages = {170-176},
   Year = {2022},
   Month = {April},
   url = {http://dx.doi.org/10.1126/science.abk1781},
   Abstract = {The mass of the <i>W</i> boson, a mediator of the weak force
             between elementary particles, is tightly constrained by the
             symmetries of the standard model of particle physics. The
             Higgs boson was the last missing component of the model.
             After observation of the Higgs boson, a measurement of the
             <i>W</i> boson mass provides a stringent test of the model.
             We measure the <i>W</i> boson mass, <i>M<sub>W</sub></i>,
             using data corresponding to 8.8 inverse femtobarns of
             integrated luminosity collected in proton-antiproton
             collisions at a 1.96 tera-electron volt center-of-mass
             energy with the CDF II detector at the Fermilab Tevatron
             collider. A sample of approximately 4 million <i>W</i> boson
             candidates is used to obtain <b>[Formula: see text]</b>, the
             precision of which exceeds that of all previous measurements
             combined (stat, statistical uncertainty; syst, systematic
             uncertainty; MeV, mega-electron volts; <i>c</i>, speed of
             light in a vacuum). This measurement is in significant
             tension with the standard model expectation.},
   Doi = {10.1126/science.abk1781},
   Key = {fds362779}
}

@article{fds332354,
   Author = {Abbott, B and Abdesselam, A and Abolins, M and Abramov, V and Acharya,
             BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon,
             TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar,
             V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler,
             M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S},
   Title = {High-[Formula Presented] jets in [Formula Presented]
             collisions at [Formula Presented] and 1800
             GeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {64},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2001},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.64.032003},
   Abstract = {Results are presented from analyses of jet data produced in
             [Formula Presented] collisions at [Formula Presented] and
             1800 GeV collected with the DØ detector during the
             1994–1995 Fermilab Tevatron Collider run. We discuss the
             details of detector calibration, and jet selection criteria
             in measurements of various jet production cross sections at
             [Formula Presented] and 1800 GeV. The inclusive jet cross
             sections, the dijet mass spectrum, the dijet angular
             distributions, and the ratio of inclusive jet cross sections
             at [Formula Presented] and 1800 GeV are compared to
             next-to-leading-order QCD predictions. The order [Formula
             Presented] calculations are in good agreement with the data.
             We also use the data at [Formula Presented] GeV to rule out
             models of quark compositeness with a contact interaction
             scale less than [Formula Presented] TeV at the [Formula
             Presented] confidence level. © 2001 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.64.032003},
   Key = {fds332354}
}

@article{fds347532,
   Author = {Sharma, M and Biswas, D and Kotwal, A and Thakuria, B and Kakati, B and Chauhan, BS and Patras, A},
   Title = {Ibuprofen-mediated reversal of fluconazole resistance in
             clinical isolates of Candida.},
   Journal = {Journal of clinical and diagnostic research :
             JCDR},
   Volume = {9},
   Number = {1},
   Pages = {DC20-DC22},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.7860/jcdr/2015/10094.5494},
   Abstract = {<h4>Introduction</h4>In view of the increasing prevalence of
             invasive Candidiasis in today's health-care scenario and the
             emergence of fluconazole resistance among clinical isolates
             of Candida, we sought to determine if Ibuprofen could elicit
             a reversal of fluconazole resistance and thereby offer a
             potential therapeutic breakthrough in fluconazole-resistant
             Candidiasis.<h4>Materials and methods</h4>We selected 69
             clinical isolates of Candida, which demonstrated an MIC of
             >32 μg/ml for fluconazole, and subjected them to broth
             microdilution in presence and absence of
             Ibuprofen.<h4>Results</h4>Forty two of the 69 isolates
             (60.9%) demonstrated reversal of Fluconazole resistance with
             concomitant use of Ibuprofen. This was characterized by
             significant species-wise variation (p=0.00008), with all the
             C. albicans isolates and none of the C. glabrata isolates
             demonstrating such reversal. Only 22.2% and 37.7% of C.
             krusei and C. tropicalis isolates respectively showed
             Ibuprofen-mediated reversal of Fluconazole
             resistance.<h4>Conclusion</h4>Since Ibuprofen is a known
             efflux pump inhibitor, our findings hint at the possible
             mechanism of Fluconazole resistance in most of our Candida
             isolates and suggest a potential therapeutic alternative
             that could be useful in the majority of Fluconazole-resistant
             clinical isolates of Candida.},
   Doi = {10.7860/jcdr/2015/10094.5494},
   Key = {fds347532}
}

@article{fds321138,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
             M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Azuma, Y and Baak, MA and Baas,
             AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus,
             M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Bedikian, S and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger,
             N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius,
             C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
             MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
             N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black,
             CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet,
             D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli,
             R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
             AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole,
             B},
   Title = {Identification and energy calibration of hadronically
             decaying tau leptons with the ATLAS experiment in pp
             collisions at [Formula: see text][Formula: see
             text].},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {303},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3500-z},
   Abstract = {This paper describes the trigger and offline reconstruction,
             identification and energy calibration algorithms for
             hadronic decays of tau leptons employed for the data
             collected from <i>pp</i> collisions in 2012 with the ATLAS
             detector at the LHC center-of-mass energy [Formula: see
             text] [Formula: see text]. The performance of these
             algorithms is measured in most cases with [Formula: see
             text] decays to tau leptons using the full 2012 dataset,
             corresponding to an integrated luminosity of 20.3
             fb[Formula: see text]. An uncertainty on the offline
             reconstructed tau energy scale of 2-4 %, depending on
             transverse energy and pseudorapidity, is achieved using two
             independent methods. The offline tau identification
             efficiency is measured with a precision of 2.5 % for
             hadronically decaying tau leptons with one associated track,
             and of 4 % for the case of three associated tracks,
             inclusive in pseudorapidity and for a visible transverse
             energy greater than 20 [Formula: see text]. For hadronic tau
             lepton decays selected by offline algorithms, the tau
             trigger identification efficiency is measured with a
             precision of 2-8 %, depending on the transverse energy. The
             performance of the tau algorithms, both offline and at the
             trigger level, is found to be stable with respect to the
             number of concurrent proton-proton interactions and has
             supported a variety of physics results using hadronically
             decaying tau leptons at ATLAS.},
   Doi = {10.1140/epjc/s10052-015-3500-z},
   Key = {fds321138}
}

@article{fds348983,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
             D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani,
             H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
             A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa,
             JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
             EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner,
             M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan,
             AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
             AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov,
             G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini,
             D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni,
             LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Bret,
             MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini,
             M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
             I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney,
             RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castelijn, R and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
             E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito,
             L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Identification and rejection of pile-up jets at high
             pseudorapidity with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {9},
   Pages = {580},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5081-5},
   Abstract = {The rejection of forward jets originating from additional
             proton-proton interactions (pile-up) is crucial for a
             variety of physics analyses at the LHC, including Standard
             Model measurements and searches for physics beyond the
             Standard Model. The identification of such jets is
             challenging due to the lack of track and vertex information
             in the pseudorapidity range | η | > 2.5 . This paper
             presents a novel strategy for forward pile-up jet tagging
             that exploits jet shapes and topological jet correlations in
             pile-up interactions. Measurements of the per-jet tagging
             efficiency are presented using a data set of 3.2 fb - 1 of
             proton-proton collisions at a centre-of-mass energy of 13
             TeV collected with the ATLAS detector. The fraction of
             pile-up jets rejected in the range 2.5 < | η | < 4.5 is
             estimated in simulated events with an average of 22
             interactions per bunch-crossing. It increases with jet
             transverse momentum and, for jets with transverse momentum
             between 20 and 50 GeV, it ranges between 49% and 67% with an
             efficiency of 85% for selecting hard-scatter jets. A case
             study is performed in Higgs boson production via the
             vector-boson fusion process, showing that these techniques
             mitigate the background growth due to additional
             proton-proton interactions, thus enhancing the reach for
             such signatures.},
   Doi = {10.1140/epjc/s10052-017-5081-5},
   Key = {fds348983}
}

@article{fds356567,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
             L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
             JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA},
   Title = {Identification of boosted Higgs bosons decaying into b-quark
             pairs with the ATLAS detector at 13 TeV},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {10},
   Year = {2019},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7335-x},
   Abstract = {This paper describes a study of techniques for identifying
             Higgs bosons at high transverse momenta decaying into
             bottom-quark pairs, H→ bb¯ , for proton–proton
             collision data collected by the ATLAS detector at the Large
             Hadron Collider at a centre-of-mass energy s=13 TeV. These
             decays are reconstructed from calorimeter jets found with
             the anti-ktR= 1.0 jet algorithm. To tag Higgs bosons, a
             combination of requirements is used: b-tagging of R= 0.2
             track-jets matched to the large-R calorimeter jet, and
             requirements on the jet mass and other jet substructure
             variables. The Higgs boson tagging efficiency and
             corresponding multijet and hadronic top-quark background
             rejections are evaluated using Monte Carlo simulation.
             Several benchmark tagging selections are defined for
             different signal efficiency targets. The modelling of the
             relevant input distributions used to tag Higgs bosons is
             studied in 36 fb- 1 of data collected in 2015 and 2016
             using g→ bb¯ and Z(→ bb¯) γ event selections in data.
             Both processes are found to be well modelled within the
             statistical and systematic uncertainties.},
   Doi = {10.1140/epjc/s10052-019-7335-x},
   Key = {fds356567}
}

@article{fds347518,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
             M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
             C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biesuz,
             NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister,
             I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
             JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet,
             D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero,
             J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman,
             JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
             S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
             K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn,
             AP},
   Title = {Identification of boosted, hadronically decaying W
             bosons and comparisons with ATLAS data taken at [Formula:
             see text] TeV.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {154},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-3978-z},
   Abstract = {This paper reports a detailed study of techniques for
             identifying boosted, hadronically decaying <i>W</i> bosons
             using 20.3 fb[Formula: see text] of proton-proton collision
             data collected by the ATLAS detector at the LHC at a
             centre-of-mass energy [Formula: see text]. A range of
             techniques for optimising the signal jet mass resolution are
             combined with various jet substructure variables. The
             results of these studies in Monte Carlo simulations show
             that a simple pairwise combination of groomed jet mass and
             one substructure variable can provide a 50 % efficiency for
             identifying <i>W</i> bosons with transverse momenta larger
             than 200 GeV while maintaining multijet background
             efficiencies of 2-4 % for jets with the same transverse
             momentum. These signal and background efficiencies are
             confirmed in data for a selection of tagging
             techniques.},
   Doi = {10.1140/epjc/s10052-016-3978-z},
   Key = {fds347518}
}

@article{fds308169,
   Author = {Kotwal, AV and Gerberich, HK and Hays, C},
   Title = {Identification of cosmic rays using drift chamber hit
             timing},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {506},
   Number = {1-2},
   Pages = {110-118},
   Publisher = {Elsevier BV},
   Year = {2003},
   Month = {June},
   url = {http://dx.doi.org/10.1016/S0168-9002(03)01371-8},
   Abstract = {Identification of cosmic rays was discussed. Drift chamber
             hit timing method was used. The central outer tracker (COT)
             tracks as cosmic rays were studied and their direction of
             propagation and time of incidence were also
             measured.},
   Doi = {10.1016/S0168-9002(03)01371-8},
   Key = {fds308169}
}

@article{fds321126,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Identification of high transverse momentum top quarks in pp
             collisions at √s= 8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2016)093},
   Abstract = {This paper presents studies of the performance of several
             jet-substructure techniques, which are used to identify
             hadronically decaying top quarks with high transverse
             momentum contained in large-radius jets. The efficiency of
             identifying top quarks is measured using a sample of
             top-quark pairs and the rate of wrongly identifying jets
             from other quarks or gluons as top quarks is measured using
             multijet events collected with the ATLAS experiment in 20.3
             fb−1of 8 TeV proton-proton collisions at the Large Hadron
             Collider. Predictions from Monte Carlo simulations are found
             to provide an accurate description of the performance. The
             techniques are compared in terms of signal efficiency and
             background rejection using simulations, covering a larger
             range in jet transverse momenta than accessible in the
             dataset. Additionally, a novel technique is developed that
             is optimized to reconstruct top quarks in events with many
             jets.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP06(2016)093},
   Key = {fds321126}
}

@article{fds307589,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert,
             B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou,
             R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
             V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia,
             A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ},
   Title = {Improved luminosity determination in pp collisions at
             [Formula: see text] using the ATLAS detector at the
             LHC.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {8},
   Pages = {2518},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2518-3},
   Abstract = {The luminosity calibration for the ATLAS detector at the LHC
             during <i>pp</i> collisions at [Formula: see text] in 2010
             and 2011 is presented. Evaluation of the luminosity scale is
             performed using several luminosity-sensitive detectors, and
             comparisons are made of the long-term stability and accuracy
             of this calibration applied to the <i>pp</i> collisions at
             [Formula: see text]. A luminosity uncertainty of [Formula:
             see text] is obtained for the 47 pb<sup>-1</sup> of data
             delivered to ATLAS in 2010, and an uncertainty of [Formula:
             see text] is obtained for the 5.5 fb<sup>-1</sup> delivered
             in 2011.},
   Doi = {10.1140/epjc/s10052-013-2518-3},
   Key = {fds307589}
}

@article{fds184837,
   Author = {A.V. Kotwal and T. Aaltonen et al [CDF Collaboration]},
   Title = {Improved Search for a Higgs Boson Produced in Association
             with Z->l+l- in proton antiproton Collisions at sqrt(s) =
             1.96 TeV},
   Journal = {Physical Review Letters},
   Year = {2010},
   Month = {Fall},
   Key = {fds184837}
}

@article{fds307893,
   Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco,
             SD and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico, M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
             R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
             S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
             MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum, W and Keung,
             J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
             M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, C and Liu, Q and Liu, T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Maksimovic, P and Malik, S and Manca, G and Manousakis-Katsikakis,
             A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson,
             ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin,
             F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shekhar, R and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki, M and Denis,
             RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
             J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini,
             N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez,
             F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang,
             T},
   Title = {Improved search for a Higgs boson produced in association
             with Z→l+l- in pp̄ collisions at
             √s=1.96TeV},
   Journal = {Physical Review Letters},
   Volume = {105},
   Number = {25},
   Pages = {251802},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.251802},
   Abstract = {We search for the standard model Higgs boson produced with a
             Z boson in 4.1fb⊃-1 of integrated luminosity collected
             with the CDF II detector at the Tevatron. In events
             consistent with the decay of the Higgs boson to a
             bottom-quark pair and the Z boson to electrons or muons, we
             set 95% credibility level upper limits on the ZH production
             cross section multiplied by the H→bb̄ branching ratio.
             Improved analysis methods enhance signal sensitivity by 20%
             relative to previous searches. At a Higgs boson mass of
             115GeV/c2 we set a limit of 5.9 times the standard model
             cross section. © 2010 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.105.251802},
   Key = {fds307893}
}

@article{fds337272,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
             VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Bolton,
             TA and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
             F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and De,
             K and Jong, SJD and Demarteau, M and Demina, R and Demine, P and Denisov,
             D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Duperrin, A and Dyshkant, A and Edmunds, D and Ellison, J and Eltzroth,
             JT and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
             T and Fein, D and Ferbel, T and Filthaut, F and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Fox, H and Frame, KC and Fu,
             S and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin,
             R and Ginther, G and Gómez, B and Goncharov, PI and Gordon, H and Goss,
             LT and Gounder, K and Goussiou, A and Graf, N and Grannis, PD and Green,
             JA and Greenlee, H and Greenwood, ZD and Grinstein, S and Groer, L and Grünendahl, S and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hall, RE and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinmiller, JM and Heinson, AP and Heintz, U and Hildreth, MD and Hirosky, R and Hobbs, JD and Hoeneisen, B and Huang, Y and Iashvili, I and Illingworth, R and Ito, AS and Jaffré, M and Jain, S and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jöstlein, H and Juste, A and Kahl, W and Kahn, S and Kajfasz, E and Kalinin, AM and Karmanov, D and Karmgard, D and Kehoe, R and Khanov, A and Kharchilava,
             A and Kim, SK and Klima, B and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kothari, B and Kotwal, AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krivkova, P and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kuznetsov, VE and Landsberg, G and Lee, WM and Leflat, A and Leggett, C and Lehner, F and Leonidopoulos, C and Li, J and Li, QZ and Lima, JGR and Lincoln, D and Linn, SL and Linnemann,
             J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AKA and Madaras, RJ and Malyshev, VL and Manankov, V and Mao,
             HS and Marshall, T and Martin, MI and Mayorov, AA and McCarthy, R and McMahon, T and Melanson, HL and Merkin, M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mokhov, N and Mondal,
             NK and Montgomery, HE and Moore, RW and Mostafa, M and Motta, HD and Mutaf,
             Y and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Naumann, NA and Neal, HA and Negret, JP and Nomerotski, A and Nunnemann, T and O'Neil,
             D and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou, K and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Peters, O and Pétroff, P and Piegaia, R and Pope, BG and Popkov, E and Prosper, HB and Protopopescu,
             S and Przybycien, MB and Qian, J and Raja, R and Rajagopalan, S and Ramberg, E and Rapidis, PA and Reay, NW and Reucroft, S and Ridel, M and Rijssenbeek, M and Rizatdinova, F and Rockwell, T and Roco, M and Royon,
             C and Rubinov, P and Ruchti, R and Rutherfoord, J and Sabirov, BM and Sajot, G and Santoro, A and Sawyer, L and Schamberger, RD and Schellman,
             H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell, RA and Simak, V and Singh, H and Sirotenko, V and Slattery, P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Song, Y and Sorín,
             V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stoker, D and Stolin, V and Stone, A and Stoyanova, DA and Strang, MA and Strauss, M and Strovink, M and Stutte, L and Sznajder, A and Talby, M and Taylor, W and Tentindo-Repond, S and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and Vaniev, V and Kooten, RV and Varelas, N and Vertogradov,
             LS and Villeneuve-Seguier, F and Volkov, AA and Vorobiev, AP and Wahl,
             HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Whiteson, D and Wijngaarden,
             DA and Willis, S and Wimpenny, SJ and Womersley, J and Wood, DR and Xu, Q and Yamada, R and Yamin, P and Yasuda, T and Yatsunenko, YA and Yip, K and Youssef, S and Yu, J and Zanabria, M and Zhang, X and Zheng, H and Zhou, B and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi,
             V and Zverev, EG and Zylberstejn, A},
   Title = {Improved W boson mass measurement with the DØ
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {66},
   Number = {1 II},
   Pages = {120011-1200118},
   Publisher = {American Physical Society (APS)},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/PhysRevD.66.012001},
   Abstract = {We have measured the W boson mass using the DØ detector and
             a data sample of 82 pb-1 from the Fermilab Tevatron
             collider. This measurement uses W→eν decays, where the
             electron is close to a boundary of a central electromagnetic
             calorimeter module. Such "edge" electrons have not been used
             in any previous DØ analysis, and represent a 14% increase
             in the W boson sample size. For these electrons, new
             response and resolution parameters are determined, and
             revised backgrounds and underlying event energy flow
             measurements are made. When the current measurement is
             combined with previous DØ W boson mass measurements, we
             obtain MW=80.483±0.084 GeV. The 8% improvement from the
             previous DØ measurement is primarily due to the improved
             determination of the response parameters for non-edge
             electrons using the sample of Z bosons with non-edge and
             edge electrons.},
   Doi = {10.1103/PhysRevD.66.012001},
   Key = {fds337272}
}

@article{fds356627,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {In situ calibration of large-radius jet energy and mass in
             13 TeV proton–proton collisions with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {2},
   Year = {2019},
   Month = {February},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-6632-8},
   Abstract = {The response of the ATLAS detector to large-radius jets is
             measured in situ using 36.2 fb- 1 of s=13 TeV proton–proton
             collisions provided by the LHC and recorded by the ATLAS
             experiment during 2015 and 2016. The jet energy scale is
             measured in events where the jet recoils against a reference
             object, which can be either a calibrated photon, a
             reconstructed Z boson, or a system of well-measured
             small-radius jets. The jet energy resolution and a
             calibration of forward jets are derived using dijet balance
             measurements. The jet mass response is measured with two
             methods: using mass peaks formed by W bosons and top quarks
             with large transverse momenta and by comparing the jet mass
             measured using the energy deposited in the calorimeter with
             that using the momenta of charged-particle tracks. The
             transverse momentum and mass responses in simulations are
             found to be about 2–3% higher than in data. This
             difference is adjusted for with a correction factor. The
             results of the different methods are combined to yield a
             calibration over a large range of transverse momenta (pT).
             The precision of the relative jet energy scale is 1–2% for
             200GeV<pT<2TeV, while that of the mass scale is 2–10%. The
             ratio of the energy resolutions in data and simulation is
             measured to a precision of 10–15% over the same pT
             range.},
   Doi = {10.1140/epjc/s10052-019-6632-8},
   Key = {fds356627}
}

@article{fds308217,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, H and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Balamurali, V and Baldin, B and Banerjee,
             S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding,
             F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey,
             D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang,
             SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger,
             C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
             P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
             G},
   Title = {Inclusive jet cross section in p̄p collisions at √ = 1.8
             TeV},
   Journal = {Physical Review Letters},
   Volume = {82},
   Number = {12},
   Pages = {2451-2456},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.82.2451},
   Abstract = {We have made a precise measurement of the central inclusive
             jet cross section at √s = 1.8 TeV. The measurement is
             based on an integrated luminosity of 92pb-1 collected at the
             Fermilab Tevatron p̄p Collider with the D0 detector. The
             cross section, reported as a function of jet transverse
             energy (ET ≥ 60 GeV) in the pseudorapidity interval |±|
             ≤ 0.5, is in good agreement with predictions from
             next-to-leading order quantum chromodynamics. © 1999 The
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.82.2451},
   Key = {fds308217}
}

@article{fds308182,
   Author = {Abbott, B and Abdesselam, A and Abolins, M and Abramov, V and Acharya,
             BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar,
             V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler,
             M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MA and Cutts, D and Davis, GA and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
             T and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin, R and Ginther,
             G and Gómez, B and Gómez, G and Goncharov, PI and González Solís,
             JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein,
             S and Groer, L and Grünendahl, S and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hou, S and Huang, Y and Illingworth, R and Ito, AS and Jaffré, M and Jerger, SA and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Karmanov, D and Karmgard, D and Kim, SK and Klima, B and Klopfenstein, C and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kuznetsov,
             VE and Landsberg, G and Leflat, A and Leggett, C and Lehner, F and Li, J and Li, QZ and Lima, JG and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AK and Madaras, RJ and Manankov, V and Mao, HS and Marshall, T and Martin, MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy, R and McDonald, J and McMahon, T and Melanson, HL and Meng,
             XC and Merkin, M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea,
             D and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery, HE and Moore,
             RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Norman, D and Nunnemann, T and Oesch, L and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou, K and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Pétroff, P and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu,
             S and Qian, J and Quintas, PZ and Raja, R and Rajagopalan, S and Ramberg,
             E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell, RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery, P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon,
             J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Strovink, M and Stutte, L and Sznajder, A and Taylor, W and Tentindo-Repond, S and Thompson, J and Toback, D and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and van Gemmeren, P and Vaniev,
             V and Van Kooten and R and Varelas, N and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Wirjawan, JV and Womersley, J and Wood, DR and Yamada, R and Yamin, P and Yasuda, T and Yip,
             K and Youssef, S and Yu, J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev,
             EG and Zylberstejn, A and D0 Collaboration},
   Title = {Inclusive jet production in pp(macro) collisions.},
   Journal = {Physical review letters},
   Volume = {86},
   Number = {9},
   Pages = {1707-1712},
   Year = {2001},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.86.1707},
   Abstract = {We report a new measurement of the pseudorapidity (eta) and
             transverse-energy ( E(T)) dependence of the inclusive jet
             production cross section in pp(macro) collisions at square
             root of s = 1.8 TeV using 95 pb(-1) of data collected with
             the D0 detector at the Fermilab Tevatron. The differential
             cross section d(2)sigma/(dE(T)d eta) is presented up to eta
             = 3, significantly extending previous measurements. The
             results are in good overall agreement with next-to-leading
             order predictions from QCD and indicate a preference for
             certain parton distribution functions.},
   Doi = {10.1103/physrevlett.86.1707},
   Key = {fds308182}
}

@article{fds308056,
   Author = {Abulencia, and A, and others},
   Title = {Inclusive search for new physics with like-sign dilepton
             events in $p \bar{p}$ collisions at $\sqrt{s}$ =
             1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {22},
   Pages = {221803},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.221803},
   Abstract = {We describe a search for anomalous production of events with
             two leptons (e or µ) of the same electric charge in
             p[overline p] collisions at a center-of-mass energy of 1.96
             TeV. Many extensions to the standard model predict the
             production of two leptons of the same electric charge. This
             search has a significant increase in sensitivity compared to
             earlier searches. Using a data sample corresponding to 1
             fb-1 of integrated luminosity recorded by the CDF II
             detector, we observe no significant excess in an inclusive
             selection (expect 33.2$\pm$4.7 events, observe 44) or in a
             supersymmetry-optimized selection (expect 7.8$\pm$1.1
             events, observe 13.)},
   Doi = {10.1103/physrevlett.98.221803},
   Key = {fds308056}
}

@article{fds307837,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S},
   Title = {Inclusive search for same-sign dilepton signatures in pp
             collisions at √s = 7 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2011},
   Number = {10},
   Pages = {1-47},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2011)107},
   Abstract = {An inclusive search is presented for new physics in events
             with two isolated leptons (e or μ) having the same electric
             charge. The data are selected from events collected from pp
             collisions at √s = 7 TeV by the ATLAS detector and
             correspond to an integrated luminosity of 34 pb-1. The
             spectra in dilepton invariant mass, missing transverse
             momentum and jet multiplicity are presented and compared to
             Standard Model predictions. In this event sample, no
             evidence is found for contributions beyond those of the
             Standard Model. Limits are set on the cross-section in a
             fiducial region for new sources of same-sign high-mass
             dilepton events in the ee, eμ and μμ channels. Four
             models predicting same-sign dilepton signals are
             constrained: two descriptions of Majorana neutrinos, a
             cascade topology similar to supersymmetry or universal extra
             dimensions, and fourth generation d-type quarks. Assuming a
             new physics scale of 1 TeV, Majorana neutrinos produced by
             an effective operator V with masses below 460 GeV are
             excluded at 95% confidence level. A lower limit of 290 GeV
             is set at 95% confidence level on the mass of fourth
             generation d-type quarks. Copyright CERN.},
   Doi = {10.1007/JHEP10(2011)107},
   Key = {fds307837}
}

@article{fds307956,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart,
             D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher,
             A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni, GP and Dionisi,
             C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
             P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
             JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
             MJ and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
             M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and da Costa, JG and Gunay-Unalan, Z and Haber, C and Hahn,
             K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Happacher,
             F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris,
             RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker,
             A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
             JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko,
             BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal,
             AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee, SW and Leone,
             S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino,
             CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín,
             R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Griso,
             SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
             G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pinera, L and Pitts,
             K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder,
             N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
             A and Ramakrishnan, V and Ranjan, N and Redondo, I and Rekovic, V and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt,
             MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider,
             FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas,
             J},
   Title = {Inclusive search for squark and gluino production in pp[over
             ] collisions at sqrt[s]=1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {12},
   Pages = {121801},
   Year = {2009},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.102.121801},
   Abstract = {We report on a search for inclusive production of squarks
             and gluinos in pp[over ] collisions at sqrt[s]=1.96 TeV, in
             events with large missing transverse energy and multiple
             jets of hadrons in the final state. The study uses a CDF Run
             II data sample corresponding to 2 fb(-1) of integrated
             luminosity. The data are in good agreement with the standard
             model predictions, giving no evidence for any squark or
             gluino component. In an R-parity conserving minimal
             supergravity scenario with A(0)=0, mu<0, and tanbeta=5, 95%
             C.L. upper limits on the production cross sections in the
             range between 0.1 and 1 pb are obtained, depending on the
             squark and gluino masses considered. For gluino masses below
             280 GeV/c(2), arbitrarily large squark masses are excluded
             at the 95% C.L., while for mass degenerate gluinos and
             squarks, masses below 392 GeV/c(2) are excluded at the 95%
             C.L.},
   Doi = {10.1103/physrevlett.102.121801},
   Key = {fds307956}
}

@article{fds307912,
   Author = {Aaltonen, and T, and others},
   Title = {Inclusive Search for Standard Model Higgs Boson Production
             in the WW Decay Channel using the CDF II
             Detector},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {6},
   Pages = {061803},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.061803},
   Abstract = {http://arxiv.org/abs/1001.4468},
   Doi = {10.1103/PhysRevLett.104.061803},
   Key = {fds307912}
}

@booklet{Adams97,
   Author = {M. R. Adams and M. Aderholz and S. Aid and P. L. Anthony and D. A. Averill and M. D. Baker and B. R. Baller and A.
             Banerjee and A. A. Bhatti and U. Bratzler and H. M. Braun and T. J. Carroll and H. L. Clark and J. M. Conrad and R.
             Davisson and I. Derado a},
   Title = {Inclusive single-particle distributions and transverse
             momenta of forward produced charged hadrons in mu p
             scattering at 470 GeV},
   Journal = {Zeitschrift Fur Physik C-particles And Fields},
   Volume = {76},
   Number = {3},
   Pages = {441 -- 463},
   Year = {1997},
   Month = {November},
   Key = {Adams97}
}

@article{fds308252,
   Author = {Adams, MR and Aderholz, M and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dietrich, FS and Dougherty, W and Dreyer, T and Eckardt,
             V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen, KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Jackson, HE and Jaffe, DE and Jancso, G and Jansen, DM and Jin, Z and Kaufmann, S and Kennedy, RD and Kinney, ER and Kobrak, HGE and Kotwal, AV and Kunori, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin, JG and Nickerson, RB and Novak, J and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou, V and Pawlik, B and Pipkin, FM and Potterveld, DH and Röser, A and Ryan, JJ and Salgado, CW and Schellman, H and Schmitt, M and Schmitz, N and Schüler, KP and Seyerlein, J and Siegert, G and Skuja,
             A and Snow, GA and Söldner-Rembold, S and Spentzouris, P and Stopa, P and Swanson, RA and Venkataramania, H and Wilhelm, M and Wilson, R and Wittek, W and Wolbers, SA and Zghiche, A and Zhao,
             T},
   Title = {Inclusive single-particle distributions and transverse
             momenta of forward produced charged hadrons in μp
             scattering at 470 GeV},
   Journal = {Zeitschrift fur Physik C-Particles and Fields},
   Volume = {76},
   Number = {3},
   Pages = {441-463},
   Publisher = {Springer Nature},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1007/s002880050567},
   Abstract = {Using data from the Fermilab fixed target experiment E665,
             general properties of forward produced charged hadrons in
             μp interactions at a primary muon energy of 470 GeV are
             investigated. The normalized inclusive single-particle
             distributions for Feynman-x D(xF) and for the transverse
             momentum D(pt2, xF) are measured as a function of W and Q2.
             The dependence of the average transverse momentum squared
             〈pt2〉 on xF, W and Q2 is studied. The increasing
             contribution from diffractive production as Q2 decreases
             leads to a reduction of the average charged hadron
             multiplicities at low (positive) xF and an enhancement at
             large xF, for Q2 ≲ 10 GeV2. It also reduces 〈pt2〉 for
             Q2 ≲ 5 GeV2 and 0.4 ≲ xF < 1.0. © Springer-Verlag
             1997.},
   Doi = {10.1007/s002880050567},
   Key = {fds308252}
}

@article{fds346200,
   Author = {Sinha, T and Karan, SC and Kotwal, A},
   Title = {Increased urinary uric acid excretion: a finding in Indian
             stone formers.},
   Journal = {Urological research},
   Volume = {38},
   Number = {1},
   Pages = {17-20},
   Year = {2010},
   Month = {February},
   url = {http://dx.doi.org/10.1007/s00240-009-0236-y},
   Abstract = {Many studies have been done to determine the risk factors
             associated with urolithiasis so that preventive measures can
             be undertaken to prevent stone formation. However the exact
             aetiology of urinary stones still remains elusive. A
             prospective control study of epidemiological factors that
             influence urinary stone formation was done to determine the
             aetiology of urinary stones. Patients with stone disease had
             a significantly higher body mass index. 24-h urine excretion
             of uric acid and phosphate was found to be significantly
             higher in stone patients as compared to controls. The intake
             of non-vegetarian food was significantly higher amongst
             stone formers. Stone patients had a significantly higher
             consumption of curd and cheese as compared to controls.
             There was a significant correlation noted between stone
             formation and a positive family and past history of stone
             disease. The results indicate that obese patients,
             especially those with a family history of stone disease,
             should be counselled on weight loss. Individuals with a past
             history of stone disease should be advised to reduce their
             dietary intake of foods rich in uric acid (meat, liver and
             beans).},
   Doi = {10.1007/s00240-009-0236-y},
   Key = {fds346200}
}

@article{fds346190,
   Author = {Yadav, AK and Kotwal, A and Gupta, H and Kulkarni, A and Verma,
             AK},
   Title = {India without Poliomyelitis: Time to Make it a
             Reality.},
   Journal = {Indian journal of community medicine : official publication
             of Indian Association of Preventive & Social
             Medicine},
   Volume = {37},
   Number = {1},
   Pages = {1-4},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.4103/0970-0218.94005},
   Doi = {10.4103/0970-0218.94005},
   Key = {fds346190}
}

@article{fds307540,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Indirect measurement of sin2θW (or MW) using μ+μ- pairs
             from γ* /Z bosons produced in p p ̄ collisions at a
             center-of-momentum energy of 1.96 TeV INDIRECT MEASUREMENT
             of sin2θW (OR ... T. AALTONEN et al.},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {7},
   Year = {2014},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.072005},
   Abstract = {Drell-Yan lepton pairs are produced in the process
             pp̄→μ+μ- +X through an intermediate γ*/Zboson. The
             forward-backward asymmetry in the polar-angle distribution
             of the μ- as a function of the invariant mass of the μ+μ-
             pair is used to obtain the effective leptonic determination
             sin2θefflept of the electroweak-mixing parameter sin2θW,
             from which the value of sin2θW is derived assuming the
             standard model. The measurement sample, recorded by the
             Collider Detector at Fermilab (CDF), corresponds to 9.2fb-1
             of integrated luminosity from pp̄ collisions at a
             center-of-momentum energy of 1.96 TeV, and is the full CDF
             Run II data set. The value of sin2θefflept is found to be
             0.2315±0. 0010, where statistical and systematic
             uncertainties are combined in quadrature. When interpreted
             within the context of the standard model using the on-shell
             renormalization scheme, where sin2θW=1-MW2/MZ2, the
             measurement yields sin2θW=0.2233±0.0009, or equivalently a
             W-boson mass of 80.365±0.047GeV/c2. The value of the
             W-boson mass is in agreement with previous determinations in
             electron-positron collisions and at the Tevatron collider.
             © 2014 American Physical Society.},
   Doi = {10.1103/PhysRevD.89.072005},
   Key = {fds307540}
}

@article{fds310399,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Indirect measurement of sin2θw (MW)
             using e+e- pairs in the Z-boson region
             with p̄p collisions at a center-of-momentum energy of 1.96
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.072002},
   Abstract = {Drell-Yan lepton pairs are produced in the process p̄p→e
             +e-+X through an intermediate γ*/Z boson. The lepton
             angular distributions are used to provide information on the
             electroweak-mixing parameter sin2θw via its observable
             effective-leptonic sin2θw, or sinâ¡2θefflept. A new
             method to infer sin 2θw or, equivalently, the W-boson mass
             MW in the on-shell scheme, is developed and tested using a
             previous CDF Run II measurement of angular distributions
             from electron pairs in a sample corresponding to 2.1 fb-1 of
             integrated luminosity from p̄p collisions at a
             center-of-momentum energy of 1.96 TeV. The value of
             sinâ¡2θefflept is found to be 0.2328±0.0011. Within a
             specified context of the standard model, this results in sin
             2θw=0.2246±0.0011, which corresponds to a W-boson mass of
             80.297±0.055 GeV/c2, in agreement with previous
             determinations in electron-position collisions and at the
             Tevatron collider. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.88.072002},
   Key = {fds310399}
}

@article{fds346194,
   Author = {Minhas, S and Kotwal, A and Singh, M},
   Title = {Infection Control in Health Care Facilities.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {67},
   Number = {1},
   Pages = {7-8},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1016/s0377-1237(11)80003-1},
   Doi = {10.1016/s0377-1237(11)80003-1},
   Key = {fds346194}
}

@article{fds346182,
   Author = {Ayub, A and Goyal, A and Kotwal, A and Kulkarni, A and Kotwal, A and Mahen,
             A},
   Title = {Infection control practices in health care: Teaching and
             learning requirements of medical undergraduates.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {69},
   Number = {2},
   Pages = {107-112},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.mjafi.2012.07.021},
   Abstract = {<h4>Background</h4>Compliance and implementation of
             infection control guidelines have been recognized as
             efficient means to prevent and control hospital acquired
             infections.<h4>Objectives</h4>To evaluate knowledge and
             practices about infection control guidelines amongst medical
             students and to explore their education needs as perceived
             by them and faculty.<h4>Methods</h4>A total of 160 final
             year students and 100 faculty members of one of the top
             medical colleges in India were selected by simple random
             sampling in each group as per sample size of 143 students
             (alpha 0.05, error 7%, prevalence 60%) and 99 (error 7.5%)
             faculty. Data collected by pilot-tested, unlinked, anonymous
             questionnaire.<h4>Results</h4>Amongst students, knowledge
             (77.50%; 95% CI, 70.24-83.72) was mixed with misconceptions.
             Only 31.25% always followed hand hygiene procedure; 50%
             recapped needles; disposal of hazardous material into
             designated containers always was low (sharps 20%,
             contaminated items 25%). Despite experiencing needle stick
             injury (6.25%) and splashes (40%), less than 30% reported
             these as 44% were unaware of reporting procedure. The
             discord between the perceptions of faculty regarding
             students and students' own perceptions was clearly evident
             (all Kappa values less than 0.50). Students and faculty
             agreed on workshops (58.13% and 58%) and reinforcement by
             colleagues (51% and 54%) but not on on-job training (51% and
             34%) and part of curriculum (48% and 40%) for
             teaching-learning infection control.<h4>Conclusion</h4>Tackling
             disconnect between students and faculty perceptions and
             empowering students with knowledge and skills in infection
             control is important. Approach needs to be researched and
             formulated as current methods seem to be
             inadequate.},
   Doi = {10.1016/j.mjafi.2012.07.021},
   Key = {fds346182}
}

@article{fds341507,
   Author = {Chekanov, SV and Beydler, M and Kotwal, AV and Gray, L and Sen, S and Tran,
             NV and Yu, SS and Zuzelski, J},
   Title = {Initial performance studies of a general-purpose detector
             for multi-TeV physics at a 100 TeV pp collider},
   Journal = {Journal of Instrumentation},
   Volume = {12},
   Number = {6},
   Year = {2017},
   Month = {June},
   url = {http://dx.doi.org/10.1088/1748-0221/12/06/P06009},
   Abstract = {This paper describes simulations of detector response to
             multi-TeV particles and jets at the Future Circular Collider
             (FCC-hh) or Super proton-proton Collider (SppC) which aim to
             collide proton beams with a centre-of-mass energy of 100
             TeV. The unprecedented energy regime of these future
             experiments imposes new requirements on detector
             technologies which can be studied using the detailed GEANT4
             simulations presented in this paper. The initial performance
             of a detector designed for physics studies at the FCC-hh or
             SppC experiments is described with an emphasis on
             measurements of single particles up to 33 TeV in transverse
             momentum. The reconstruction of hadronic jets has also been
             studied in the transverse momentum range from 50 GeV to 26
             TeV. The granularity requirements for calorimetry are
             investigated using the two-particle spatial resolution
             achieved for hadron showers.},
   Doi = {10.1088/1748-0221/12/06/P06009},
   Key = {fds341507}
}

@article{fds346218,
   Author = {Kotwal, A and Priya, R and Thakur, R and Gupta, V and Kotwal, J and Seth,
             T},
   Title = {Injection practices in a metropolis of North India:
             perceptions, determinants and issues of safety.},
   Journal = {Indian journal of medical sciences},
   Volume = {58},
   Number = {8},
   Pages = {334-344},
   Year = {2004},
   Month = {August},
   Abstract = {<h4>Background</h4>At least 50 percent of the injections
             administered each year are unsafe, more particularly in
             developing countries, posing serious health risks. An
             initial assessment to describe injection practices; their
             determinants and adverse effects can prevent
             injection-associated transmission of blood borne pathogens
             by reducing injection frequency and adoption of safe
             injection practices.<h4>Aims</h4>To assess the injection
             practices in a large metropolitan city encompassing varied
             socio-cultural scenarios. STUDY SETTING AND DESIGN: Field
             based cross sectional survey covering urban non-slum, slum
             and peri-urban areas of a large metropolitan
             city.<h4>Methods and material</h4>Injection prescribers,
             providers and community members selected by random sampling
             from the study areas. Pre tested questionnaires assessed
             knowledge and perceptions of study subjects towards
             injections and their possible complications. Observation of
             the process of injection and prescription audit also carried
             out.<h4>Statistical analysis</h4>MS Access for database and
             SPSS ver 11 for analysis. Point estimates, 95% confidence
             intervals, Chi Square, t test, one-way ANOVA.<h4>Results</h4>The
             per capita injection rate was 5.1 per year and ratio of
             therapeutic to immunization injections was 4.4:1. Only
             22.5%of injections were administered with a sterile syringe
             and needle. The level of knowledge about HIV and HBV
             transmission by unsafe injections was satisfactory amongst
             prescribers and community, but inadequate amongst providers.
             HCV was known to a very few in all the groups. The annual
             incidence of needle stick injuries among providers was quite
             high.<h4>Conclusion</h4>A locally relevant safe injection
             policy based on multi disciplinary approach is required to
             reduce number of injections, unsafe injections and their
             attendant complications.},
   Key = {fds346218}
}

@article{fds346199,
   Author = {Kotwal, A},
   Title = {Injections need for reduction, safety and
             appropriateness.},
   Journal = {Indian pediatrics},
   Volume = {47},
   Number = {5},
   Pages = {399-400},
   Year = {2010},
   Month = {May},
   url = {http://dx.doi.org/10.1007/s13312-010-0071-9},
   Doi = {10.1007/s13312-010-0071-9},
   Key = {fds346199}
}

@article{fds346215,
   Author = {Kotwal, A},
   Title = {Innovation, diffusion and safety of a medical technology: a
             review of the literature on injection practices.},
   Journal = {Social science & medicine (1982)},
   Volume = {60},
   Number = {5},
   Pages = {1133-1147},
   Year = {2005},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.socscimed.2004.06.044},
   Abstract = {The rapid uptake of the hypodermic syringe as a medical
             technology by physicians in Europe and America since its
             introduction in the middle of the 19th century has led to a
             level of medical and public acceptance seldom reached by
             other therapeutic techniques. Presently, the developed world
             has clear guidelines regarding injection use and safety; in
             contrast, developing countries are facing the brunt of risks
             associated with the use of this technology, which was
             introduced into their societies during the early 20th
             century. There is now a popular demand for injections, and
             an alarming number of unnecessary and unsafe injections are
             being administered. The problem of unsafe injections is not
             restricted to curative injections, but includes
             immunizations too. The association of unsafe injections and
             infection transmission is quite clear, and there is an
             urgent need to reduce the number of required injections and
             make them safe. An understanding of the determinants of
             current injection practices in the socio-cultural-economic
             context is necessary in order to plan relevant and effective
             interventions.},
   Doi = {10.1016/j.socscimed.2004.06.044},
   Key = {fds346215}
}

@article{fds346181,
   Author = {Kotwal, A},
   Title = {Innovations in teaching/learning methods for medical
             students: research with mentoring.},
   Journal = {Indian journal of public health},
   Volume = {57},
   Number = {3},
   Pages = {144-146},
   Year = {2013},
   Month = {July},
   url = {http://dx.doi.org/10.4103/0019-557x.119822},
   Abstract = {In this era of evidence-based medicine, innovative teaching
             learning methods coupled with appropriate mentoring are
             required to make the undergraduate medical students
             interested in the speciality of Community Medicine. Teaching
             research methodology to medical students by a hands-on
             approach along with mentoring by involving them in small,
             feasible, sustainable, and replicable studies on a topic of
             interest clearly showed renewed interest among students
             toward the subject.},
   Doi = {10.4103/0019-557x.119822},
   Key = {fds346181}
}

@article{fds308157,
   Author = {Hays, C and Huang, Y and Kotwal, AV and Gerberich, HK and Menzemer, S and Rinnert, K and Lecci, C and Herndon, M and Snider,
             FD},
   Title = {Inside-out tracking at CDF},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {538},
   Number = {1-3},
   Pages = {249-254},
   Publisher = {Elsevier BV},
   Year = {2005},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.nima.2004.08.104},
   Abstract = {The Central Outer Tracker (COT) at the Collider Detector at
             Fermilab (CDF) is used to reconstruct charged particles in
             the central rapidity region. The silicon tracker is used to
             improve the central track measurement and to reconstruct
             charged particles in the forward rapidity region. We
             describe the inside-out tracking algorithm, which improves
             the track measurement in the intermediate rapidity region by
             attaching COT hits to reconstructed silicon tracks. © 2004
             Elsevier B.V. All rights reserved.},
   Doi = {10.1016/j.nima.2004.08.104},
   Key = {fds308157}
}

@article{fds30153,
   Author = {Christopher Hays and Yimei Huang and Ashutosh V. Kotwal and Heather
             K. Gerberich and Stephanie Menzemer and Kurt Rinnert and Claudia
             Lecci, Matthew Herndon and Frederick D. Snider},
   Title = {Inside-out tracking at CDF},
   Journal = {Nuclear Instruments and Methods in Physics Research Section
             A},
   Year = {2004},
   Month = {September},
   Key = {fds30153}
}

@article{fds374212,
   Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk
             Cakir, I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Castillo, FL and Costanza, F and Delmastro, M and Di
             Ciaccio, L and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo
             Martinez, N and Poddar, G and Sanchez Pineda and A and Sauvan, E and Bernardi, G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Li, T and Marchiori, G and Nakkalil, K and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wamorkar, T and Wang, R and Zhang, J and Cheu, E and Cui, Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Tost,
             M},
   Title = {Integrated and differential fiducial cross-section
             measurements for the vector boson fusion production of the
             Higgs boson in the H →WW∗→eνμν decay channel at 13
             TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {108},
   Number = {7},
   Year = {2023},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.108.072003},
   Abstract = {The vector-boson production cross section for the Higgs
             boson decay in the Formula Presented channel is measured as
             a function of kinematic observables sensitive to the Higgs
             boson production and decay properties as well as integrated
             in a fiducial phase space. The analysis is performed using
             the proton-proton collision data collected by the ATLAS
             detector in Run 2 of the LHC at Formula Presented
             center-of-mass energy, corresponding to an integrated
             luminosity of Formula Presented. The different flavor final
             state is studied by selecting an electron and a muon
             originating from a pair of Formula Presented bosons and
             compatible with the Higgs boson decay. The data are
             corrected for the effects of detector inefficiency and
             resolution, and the measurements are compared with different
             state-of-the-art theoretical predictions. The differential
             cross sections are used to constrain anomalous interactions
             described by dimension-six operators in an effective field
             theory.},
   Doi = {10.1103/PhysRevD.108.072003},
   Key = {fds374212}
}

@article{fds307848,
   Author = {Aaltonen, and T, and al, E},
   Title = {Invariant Mass Distribution of Jet Pairs Produced in
             Association with a ${W}$ Boson in $p\overline{p}$ Collisions
             at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {17},
   Pages = {171801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.171801},
   Abstract = {We report a study of the invariant mass distribution of jet
             pairs produced in association with a W boson using data
             collected with the CDF detector which correspond to an
             integrated luminosity of 4.3  fb(-1). The observed
             distribution has an excess in the 120-160  GeV/c(2) mass
             range which is not described by current theoretical
             predictions within the statistical and systematic
             uncertainties. In this Letter, we report studies of the
             properties of this excess.},
   Doi = {10.1103/PhysRevLett.106.171801},
   Key = {fds307848}
}

@article{fds307536,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Invariant-mass distribution of jet pairs produced in
             association with a W boson in p p ̄ collisions at s
             =1.96TeV using the full CDF Run II data set invariant-mass
             distribution of ⋯ T. Aaltonen et al.},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {9},
   Year = {2014},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.092001},
   Abstract = {We report on a study of the dijet invariant-mass
             distribution in events with one identified lepton, a
             significant imbalance in the total event transverse
             momentum, and two jets. This distribution is sensitive to
             the possible production of a new particle in association
             with a W boson, where the boson decays leptonically. We use
             the full data set of proton-antiproton collisions at 1.96
             TeV center-of-mass energy collected by the Collider Detector
             at the Fermilab Tevatron, corresponding to an integrated
             luminosity of 8.9fb-1. The data are found to be consistent
             with standard model expectations, and a 95% confidence level
             upper limit is set on the production cross section of a W
             boson in association with a new particle decaying into two
             jets. © 2014 American Physical Society.},
   Doi = {10.1103/PhysRevD.89.092001},
   Key = {fds307536}
}

@article{fds346196,
   Author = {Kotwal, A},
   Title = {Iodine deficiency disorders: a health policy and planning
             perspective.},
   Journal = {Indian journal of public health},
   Volume = {54},
   Number = {4},
   Pages = {175-178},
   Year = {2010},
   Month = {October},
   url = {http://dx.doi.org/10.4103/0019-557x.77255},
   Doi = {10.4103/0019-557x.77255},
   Key = {fds346196}
}

@article{fds308203,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson,
             EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buescher,
             V and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum,
             Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev,
             SV and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
             K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
             SP and Diehl, HT and Diesburg, M and di Loreto, G and Draper, P and Ducros,
             Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison,
             J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
             T and Feher, S and Fein, D and Ferbel, T},
   Title = {Isolated photon cross section in p p̄ collisions at √s =
             1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {84},
   Number = {13},
   Pages = {2786-2791},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevLett.84.2786},
   Abstract = {We report a new measurement of the cross section for the
             production of isolated photons with transverse energies (E
             Tγ) above 10 GeV and pseudorapidities |η| < 2.5 in p̄
             collisions at √s = 1.8 TeV. The results are based on a
             data sample of 107.6 pb -1 recorded during 1992-1995 with
             the D0 detector at the Fermilab Tevatron collider. The
             background, predominantly from jets which fragment to
             neutral mesons, was estimated using the longitudinal shower
             shape of photon candidates in the calorimeter. The measured
             cross section is in good agreement with the next-to-leading
             order QCD calculation for E Tγ ≳ 36 GeV. © 2000 The
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.84.2786},
   Key = {fds308203}
}

@article{fds310309,
   Author = {Atlas Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
             J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
             E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
             N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
             R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat,
             P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes,
             GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
             V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
             J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
             P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger,
             K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burghgrave,
             B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey,
             P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar,
             CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
             B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Chouridou, S and Chow, BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH},
   Title = {Jet energy measurement and its systematic uncertainty in
             proton-proton collisions at [Formula: see text] TeV with
             the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Pages = {17},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3190-y},
   Abstract = {The jet energy scale (JES) and its systematic uncertainty
             are determined for jets measured with the ATLAS detector
             using proton-proton collision data with a centre-of-mass
             energy of [Formula: see text] TeV corresponding to an
             integrated luminosity of [Formula: see text][Formula: see
             text]. Jets are reconstructed from energy deposits forming
             topological clusters of calorimeter cells using the
             anti-[Formula: see text] algorithm with distance parameters
             [Formula: see text] or [Formula: see text], and are
             calibrated using MC simulations. A residual JES correction
             is applied to account for differences between data and MC
             simulations. This correction and its systematic uncertainty
             are estimated using a combination of in situ techniques
             exploiting the transverse momentum balance between a jet and
             a reference object such as a photon or a [Formula: see text]
             boson, for [Formula: see text] and pseudorapidities
             [Formula: see text]. The effect of multiple proton-proton
             interactions is corrected for, and an uncertainty is
             evaluated using in situ techniques. The smallest JES
             uncertainty of less than 1 % is found in the central
             calorimeter region ([Formula: see text]) for jets with
             [Formula: see text]. For central jets at lower [Formula: see
             text], the uncertainty is about 3 %. A consistent JES
             estimate is found using measurements of the calorimeter
             response of single hadrons in proton-proton collisions and
             test-beam data, which also provide the estimate for
             [Formula: see text] TeV. The calibration of forward jets is
             derived from dijet [Formula: see text] balance measurements.
             The resulting uncertainty reaches its largest value of 6 %
             for low-[Formula: see text] jets at [Formula: see text].
             Additional JES uncertainties due to specific event
             topologies, such as close-by jets or selections of event
             samples with an enhanced content of jets originating from
             light quarks or gluons, are also discussed. The magnitude of
             these uncertainties depends on the event sample used in a
             given physics analysis, but typically amounts to
             0.5-3 %.},
   Doi = {10.1140/epjc/s10052-014-3190-y},
   Key = {fds310309}
}

@article{fds307621,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Aktas, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A},
   Title = {Jet energy measurement with the ATLAS detector in
             proton-proton collisions at √s =7 TeV},
   Journal = {European Physical Journal C},
   Volume = {73},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2304-2},
   Abstract = {The jet energy scale and its systematic uncertainty are
             determined for jets measured with the ATLAS detector at the
             LHC in proton-proton collision data at a centre-of-mass
             energy of √ s = 7 TeV corresponding to an integrated
             luminosity of 38 pb-1. Jets are reconstructed with the
             anti-kt algorithm with distance parameters R = 0.4 or R =
             0.6. Jet energy and angle corrections are determined from
             Monte Carlo simulations to calibrate jets with transverse
             momenta pT ≥ 20 GeV and pseudorapidities |η| < 4.5. The
             jet energy systematic uncertainty is estimated using the
             single isolated hadron response measured in situ and in
             test-beams, exploiting the transverse momentum balance
             between central and forward jets in events with dijet
             topologies and studying systematic variations in Monte Carlo
             simulations. The jet energy uncertainty is less than 2.5 %
             in the central calorimeter region (|η| < 0.8) for jets with
             60 ≤ pT < 800 GeV, and is maximally 14 % for pT ≤ 30 GeV
             in the most forward region 3.2 ≤ |η| < 4.5. The jet
             energy is validated for jet transverse momenta up to 1 TeV
             to the level of a few percent using several in situ
             techniques by comparing a well-known reference such as the
             recoiling photon pT, the sum of the transverse momenta of
             tracks associated to the jet, or a system of low-pT jets
             recoiling against a high-pT jet. More sophisticated jet
             calibration schemes are presented based on calorimeter cell
             energy density weighting or hadronic properties of jets,
             aiming for an improved jet energy resolution and a reduced
             flavour dependence of the jet response. The systematic
             uncertainty of the jet energy determined from a combination
             of in situ techniques is consistent with the one derived
             from single hadron response measurements over a wide
             kinematic range. The nominal corrections and uncertainties
             are derived for isolated jets in an inclusive sample of
             high-pT jets. Special cases such as event topologies with
             close-by jets, or selections of samples with an enhanced
             content of jets originating from light quarks, heavy quarks
             or gluons are also discussed and the corresponding
             uncertainties are determined.},
   Doi = {10.1140/epjc/s10052-013-2304-2},
   Key = {fds307621}
}

@article{fds307615,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
             A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG},
   Title = {Jet energy resolution in proton-proton collisions at
             [Formula: see text] recorded in 2010 with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {3},
   Pages = {2306},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2306-0},
   Abstract = {The measurement of the jet energy resolution is presented
             using data recorded with the ATLAS detector in proton-proton
             collisions at [Formula: see text]. The sample corresponds to
             an integrated luminosity of 35 pb<sup>-1</sup>. Jets are
             reconstructed from energy deposits measured by the
             calorimeters and calibrated using different jet calibration
             schemes. The jet energy resolution is measured with two
             different in situ methods which are found to be in agreement
             within uncertainties. The total uncertainties on these
             measurements range from 20 % to 10 % for jets within
             |<i>y</i>|<2.8 and with transverse momenta increasing
             from 30 GeV to 500 GeV. Overall, the Monte Carlo
             simulation of the jet energy resolution agrees with the data
             within 10 %.},
   Doi = {10.1140/epjc/s10052-013-2306-0},
   Key = {fds307615}
}

@article{fds358460,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
             KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
   Title = {Jet energy scale and resolution measured in proton–proton
             collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {8},
   Year = {2021},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09402-3},
   Abstract = {Jet energy scale and resolution measurements with their
             associated uncertainties are reported for jets using
             36–81 fb- 1 of proton–proton collision data with a
             centre-of-mass energy of s=13 TeV collected by the ATLAS
             detector at the LHC. Jets are reconstructed using two
             different input types: topo-clusters formed from energy
             deposits in calorimeter cells, as well as an algorithmic
             combination of charged-particle tracks with those
             topo-clusters, referred to as the ATLAS particle-flow
             reconstruction method. The anti-kt jet algorithm with radius
             parameter R= 0.4 is the primary jet definition used for both
             jet types. This result presents new jet energy scale and
             resolution measurements in the high pile-up conditions of
             late LHC Run 2 as well as a full calibration of
             particle-flow jets in ATLAS. Jets are initially calibrated
             using a sequence of simulation-based corrections. Next,
             several in situ techniques are employed to correct for
             differences between data and simulation and to measure the
             resolution of jets. The systematic uncertainties in the jet
             energy scale for central jets (| η| < 1.2) vary from 1% for
             a wide range of high-pT jets (250<pT<2000GeV), to 5% at very
             low pT (20GeV) and 3.5% at very high pT (>2.5TeV). The
             relative jet energy resolution is measured and ranges from
             (24 ± 1.5)% at 20 GeV to (6 ± 0.5)% at
             300 GeV.},
   Doi = {10.1140/epjc/s10052-021-09402-3},
   Key = {fds358460}
}

@article{fds356729,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Jet energy scale measurements and their systematic
             uncertainties in proton-proton collisions at s =13 TeV with
             the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {96},
   Number = {7},
   Year = {2017},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.96.072002},
   Abstract = {Jet energy scale measurements and their systematic
             uncertainties are reported for jets measured with the ATLAS
             detector using proton-proton collision data with a
             center-of-mass energy of s=13 TeV, corresponding to an
             integrated luminosity of 3.2 fb-1 collected during 2015 at
             the LHC. Jets are reconstructed from energy deposits forming
             topological clusters of calorimeter cells, using the anti-kt
             algorithm with radius parameter R=0.4. Jets are calibrated
             with a series of simulation-based corrections and in situ
             techniques. In situ techniques exploit the transverse
             momentum balance between a jet and a reference object such
             as a photon, Z boson, or multijet system for jets with
             20<pT<2000 GeV and pseudorapidities of |η|<4.5, using both
             data and simulation. An uncertainty in the jet energy scale
             of less than 1% is found in the central calorimeter region
             (|η|<1.2) for jets with 100<pT<500 GeV. An uncertainty of
             about 4.5% is found for low-pT jets with pT=20 GeV in the
             central region, dominated by uncertainties in the
             corrections for multiple proton-proton interactions. The
             calibration of forward jets (|η|>0.8) is derived from dijet
             pT balance measurements. For jets of pT=80 GeV, the
             additional uncertainty for the forward jet calibration
             reaches its largest value of about 2% in the range |η|>3.5
             and in a narrow slice of 2.2<|η|<2.4.},
   Doi = {10.1103/PhysRevD.96.072002},
   Key = {fds356729}
}

@article{fds307776,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Jet mass and substructure of inclusive jets in √s = 7TeV
             pp collisions with the ATLAS experiment},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP05(2012)128},
   Abstract = {Recent studies have highlighted the potential of jet
             substructure techniques to identify the hadronic decays of
             boosted heavy particles. These studies all rely upon the
             assumption that the internal substructure of jets generated
             by QCD radiation is well understood. In this article, this
             assumption is tested on an inclusive sample of jets recorded
             with the ATLAS detector in 2010, which corresponds to 35 pb
             -1 of pp collisions delivered by the LHC at Rs =
             7TeV.},
   Doi = {10.1007/JHEP05(2012)128},
   Key = {fds307776}
}

@article{fds347508,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Santos,
             SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Billoud, TRV and Bilokon, H and Bindi, M and Bingul,
             A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard,
             DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair,
             RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger,
             AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr,
             JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
             JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Bret,
             MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini,
             M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
             I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney,
             RMD and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carvalho,
             J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
             A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN},
   Title = {Jet reconstruction and performance using particle flow with
             the ATLAS Detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {7},
   Pages = {466},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5031-2},
   Abstract = {This paper describes the implementation and performance of a
             particle flow algorithm applied to 20.2 fb[Formula: see
             text] of ATLAS data from 8 TeV proton-proton collisions in
             Run 1 of the LHC. The algorithm removes calorimeter energy
             deposits due to charged hadrons from consideration during
             jet reconstruction, instead using measurements of their
             momenta from the inner tracker. This improves the accuracy
             of the charged-hadron measurement, while retaining the
             calorimeter measurements of neutral-particle energies. The
             paper places emphasis on how this is achieved, while
             minimising double-counting of charged-hadron signals between
             the inner tracker and calorimeter. The performance of
             particle flow jets, formed from the ensemble of signals from
             the calorimeter and the inner tracker, is compared to that
             of jets reconstructed from calorimeter energy deposits
             alone, demonstrating improvements in resolution and pile-up
             stability.},
   Doi = {10.1140/epjc/s10052-017-5031-2},
   Key = {fds347508}
}

@article{fds349662,
   Author = {Yeh, CH and Chekanov, SV and Kotwal, AV and Proudfoot, J and Sen, S and Tran, NV and Yu, SS},
   Title = {Jet substructure variables with the SiFCC detector at 100
             TeV},
   Journal = {Proceedings of Science},
   Volume = {340},
   Year = {2019},
   Month = {January},
   Abstract = {Future experiments beyond the LHC era will measure
             high-momentum bosons (W, Z, H) and top quarks with strongly
             collimated decay products that form hadronic jets. This
             paper describes the studies of the performance of jet
             substructure variables using the Geant4 simulation of a
             detector designed for high energy pp collisions at a 100 TeV
             collider. The two-prong jets from Z′ → WW and
             three-prong jets from Z′ → tt&tild; are compared with
             the background from light quark jets, assuming Z′ masses
             in the range 5 - 40 TeV. Our results indicate that the
             performance of jetsubstructure reconstruction improves with
             reducing transverse cell sizes of a hadronic calorimeter
             from Δη × Δφ = 0:087×0:087 to 0:022×0:022 in most
             cases.},
   Key = {fds349662}
}

@article{fds364960,
   Author = {Bonilla, J and Chachamis, G and Dillon, BM and Chekanov, SV and Erbacher, R and Gouskos, L and Hinzmann, A and Höche, S and Huffman,
             BT and Kotwal, AV and Kar, D and Kogler, R and Lange, C and LeBlanc, M and Lemmon, R and McLean, C and Nachman, B and Neubauer, MS and Plehn, T and Rappoccio, S and Roy, D and Roloff, J and Stark, G and Tran, N and Vos, M and Yeh, C-H and Yu, S-S},
   Title = {Jets and Jet Substructure at Future Colliders},
   Journal = {Frontiers in Physics},
   Volume = {10},
   Publisher = {Frontiers Media SA},
   Year = {2022},
   Month = {June},
   url = {http://dx.doi.org/10.3389/fphy.2022.897719},
   Abstract = {<jats:p>Even though jet substructure was not an original
             design consideration for the Large Hadron Collider (LHC)
             experiments, it has emerged as an essential tool for the
             current physics program. We examine the role of jet
             substructure on the motivation for and design of future
             energy Frontier colliders. In particular, we discuss the
             need for a vibrant theory and experimental research and
             development program to extend jet substructure physics into
             the new regimes probed by future colliders. Jet substructure
             has organically evolved with a close connection between
             theorists and experimentalists and has catalyzed exciting
             innovations in both communities. We expect such developments
             will play an important role in the future energy Frontier
             physics program.</jats:p>},
   Doi = {10.3389/fphy.2022.897719},
   Key = {fds364960}
}

@article{fds307745,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni,
             G and Arutinov, D},
   Title = {Ks0 and Λ production in pp interactions at √s=0.9 and 7
             TeV measured with the ATLAS detector at the
             LHC},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012001},
   Abstract = {The production of KS0 and Λ hadrons is studied in pp
             collision data at √s=0.9 and 7 TeV collected with the
             ATLAS detector at the LHC using a minimum-bias trigger. The
             observed distributions of transverse momentum, rapidity, and
             multiplicity are corrected to hadron level in a
             model-independent way within well-defined phase-space
             regions. The distribution of the production ratio of Λ̄ to
             Λ baryons is also measured. The results are compared with
             various Monte Carlo simulation models. Although most of
             these models agree with data to within 15% in the KS0
             distributions, substantial disagreements are found in the Λ
             distributions of transverse momentum. © 2012
             CERN.},
   Doi = {10.1103/PhysRevD.85.012001},
   Key = {fds307745}
}

@article{fds347520,
   Author = {Kotwal, A},
   Title = {Letter to the Editor.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {72},
   Number = {1},
   Pages = {95-96},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.mjafi.2015.10.003},
   Doi = {10.1016/j.mjafi.2015.10.003},
   Key = {fds347520}
}

@article{fds310387,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau,
             M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli,
             F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura,
             AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
             FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
             MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov,
             AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
             JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
             S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
             IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Light-quark and gluon jet discrimination in [Formula: see
             text] collisions at [Formula: see text] with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {8},
   Pages = {3023},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3023-z},
   Abstract = {A likelihood-based discriminant for the identification of
             quark- and gluon-initiated jets is built and validated using
             4.7 fb[Formula: see text] of proton-proton collision data
             at [Formula: see text] [Formula: see text] collected with
             the ATLAS detector at the LHC. Data samples with enriched
             quark or gluon content are used in the construction and
             validation of templates of jet properties that are the input
             to the likelihood-based discriminant. The discriminating
             power of the jet tagger is established in both data and
             Monte Carlo samples within a systematic uncertainty of
             [Formula: see text] 10-20 %. In data, light-quark jets can
             be tagged with an efficiency of [Formula: see text] while
             achieving a gluon-jet mis-tag rate of [Formula: see text] in
             a [Formula: see text] range between [Formula: see text] and
             [Formula: see text] for jets in the acceptance of the
             tracker. The rejection of gluon-jets found in the data is
             significantly below what is attainable using a Pythia 6
             Monte Carlo simulation, where gluon-jet mis-tag rates of
             10 % can be reached for a 50 % selection efficiency of
             light-quark jets using the same jet properties.},
   Doi = {10.1140/epjc/s10052-014-3023-z},
   Key = {fds310387}
}

@article{fds307841,
   Author = {Aaltonen, and T, and al, E},
   Title = {Limits on Anomalous Trilinear Gauge Couplings in ${Z}\gamma$
             Events from $p\overline{p}$ Collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {5},
   Pages = {051802},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.051802},
   Abstract = {Using Zγ candidate events collected by the CDF detector at
             the Tevatron Collider, we search for potential anomalous
             (non-standard-model) couplings between the Z boson and the
             photon. Zγ couplings vanish at tree level and are heavily
             suppressed at higher orders; hence any evidence of couplings
             indicates new physics. Measurements are performed using data
             corresponding to an integrated luminosity of 4.9  fb(-1)
             in the Z→νν¯ decay channel and 5.1  fb(-1) in the
             Z→l(+)l(-) (l=μ, e) decay channels. The combination of
             these measurements provides the most stringent limits to
             date on Zγ trilinear gauge couplings. Using an energy scale
             of Λ=1.5  TeV to allow for a direct comparison with
             previous measurements, we find limits on the CP-conserving
             parameters that describe Zγ couplings to be
             |h(3)(γ,Z)|<0.022 and |h(4)(γ,Z)|<0.0009. These results
             are consistent with standard model predictions.},
   Doi = {10.1103/PhysRevLett.107.051802},
   Key = {fds307841}
}

@article{fds308064,
   Author = {Aaltonen, T and Abulencia, A and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev,
             K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Behari,
             S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak,
             M},
   Title = {Limits on anomalous triple gauge couplings in pp̄
             collisions at s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {76},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.76.111103},
   Abstract = {We present a search for anomalous triple gauge couplings
             (ATGC) in WW and WZ boson production. The boson pairs are
             produced in pp̄ collisions at s=1.96TeV, and the data
             sample corresponds to 350pb-1 of integrated luminosity
             collected with the CDF II detector at the Fermilab Tevatron.
             In this search one W decays to leptons, and the other boson
             (W or Z) decays hadronically. Combining with a previously
             published CDF measurement of Wγ boson production yields
             ATGC limits of -0.18<λ<0.17 and -0.46<Δκ<0.39 at the 95%
             confidence level, using a cutoff scale Λ=1.5TeV. © 2007
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.76.111103},
   Key = {fds308064}
}

@booklet{Abbott98d,
   Author = {B. Abbott and M. Abolins and B. S. Acharya and I. Adam and D. L. Adams and M. Adams and S. Ahn and H. Aihara and G. A.
             Alves and N. Amos and E. W. Anderson and R. Astur and M. M.
             Baarmand and L. Babukhadia and A. Baden and V. Balamurali and J. Balderston},
   Title = {Limits on anomalous WW gamma and WWZ couplings},
   Journal = {Physical Review D},
   Volume = {5803},
   Number = {3},
   Year = {1998},
   Month = {August},
   Key = {Abbott98d}
}

@article{fds308201,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson,
             EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Brooijmans, G and Brass, A and Buchholz, D and Buescher,
             V and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum,
             Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev,
             SV and Chen, LP and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Connolly, B and Cooper,
             WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein,
             D},
   Title = {Limits on anomalous WWγ and WWZ couplings from WW/WZ→e
             vjj production},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {62},
   Number = {5},
   Pages = {1-18},
   Year = {2000},
   Month = {September},
   Abstract = {Limits on anomalous WWγ and WWZ couplings are presented
             from a study of WW/WZ→e vjj events produced in pp̄
             collisions at √s=1.8 TeV. Results from the analysis of
             data collected using the DØ detector during the 1993-1995
             Tevatron collider run at Fermilab are combined with those of
             an earlier study from the 1992-1993 run. A fit to the
             transverse momentum spectrum of the W boson yields direct
             limits on anomalous WWγ and WWZ couplings. With the
             assumption that the WWγ and WWZ couplings are equal, we
             obtain -0.34<λ<0.36 (with Δκ=0) and -0.43<Δκ<0.59 (with
             λ=0) at the 95% confidence level for a form-factor scale
             Λ=2.0 TeV. ©2000 The American Physical
             Society.},
   Key = {fds308201}
}

@booklet{Abachi97d,
   Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Álvarez, G and Alves,
             GA and Amidi, E and Amos, N and Anderson, EW and Aronson, SH and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Bendich, J and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Bischoff, A and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt,
             A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty,
             D and Chang, S-M and Chekulaev, SV and Chen, L-P and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
             C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and De,
             K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard,
             J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahey, S and Fahland, T and Fatyga, M and Fatyga, MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE and Fortner, M and Frame, KC and Franzini, P and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Geld, TL and Genik II and RJ and Genser, K and Gerber, CE and Gibbard, B and Glebov, V and Glenn, S and Gobbi, B and Goforth, M and Goldschmidt, A and Gómez, B and Gomez, G and Goncharov,
             PI and González Solís and JL and Gordon, H and Goss, LT and Goussiou, A and Graf, N and Grannis, PD and Green, DR and Green, J and Greenlee, H and Griffin, G and Grim, G and Grossman, N and Grudberg, P and Grünendahl,
             S and Guglielmo, G and Guida, JA and Guida, JM and Guryn, W and Gurzhiev,
             SN and Gutierrez, P and Gutnikov, YE and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hansen, S and Hauptman, JM and Hedin, D and Heinson, AP and Heintz, U and Hernández-Montoya, R and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hsieh, F and Hu, T and Hu, T and Huehn, T and Ito, AS and James, E and Jaques, J and Jerger, SA and Jiang, JZ-Y and Joffe-Minor, T and Johns, K and Johnson, M and Jonckheere, A and Jones,
             M and Jöstlein, H and Jun, SY and Jung, CK and Kahn, S and Kalbfleisch, G and Kang, JS and Kehoe, R and Kelly, ML and Kerth, L and Kim, CL and Kim, SK and Klatchko, A and Klima, B and Klochkov, BI and Klopfenstein, C and Klyukhin, VI and Kochetkov, VI and Kohli, JM and Koltick, D and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kourlas, J and Kozelov, AV and Kozlovski, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kunori, S and Lami, S and Lan, H and Landsberg, G and Lauer, B and Lebrat, J-F and Leflat, A and Li, H and Li, J and Li, YK and Li-Demarteau, QZ and Lima, JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Liu, Q and Liu, YC and Lobkowicz, F and Loken, SC and Lökös, S and Lueking, L and Lyon, AL and Maciel, AKA and Madaras, RJ and Madden, R and Magaña-Mendoza, L and Mani, S and Mao,
             HS and Markeloff, R and Markosky, L and Marshall, T and Martin, MI and May,
             B and Mayorov, AA and McCarthy, R and McDonald, J and McKibben, T and McKinley, J and McMahon, T and Melanson, HL and Merritt, KW and Miettinen, H and Mincer, A and de Miranda, JM and Mishra, CS and Mokhov,
             N and Mondal, NK and Montgomery, HE and Mooney, P and da Motta, H and Mudan, M and Murphy, C and Nang, F and Narain, M and Narasimham, VS and Narayanan, A and Neal, HA and Negret, JP and Nemethy, P and Nes̆ić, D and Nicola, M and Norman, D and Oesch, L and Oguri, V and Oltman, E and Oshima,
             N and Owen, D and Padley, P and Pang, M and Para, A and Park, YM and Partridge, R and Parua, N and Paterno, M and Perkins, J and Peters, M and Piekarz, H and Pischalnikov, Y and Podstavkov, VM and Pope, BG and Prosper, HB and Protopopescu, S and Pus̆eljić, D and Qian, J and Quintas, PZ and Raja, R and Rajagopalan, S and Ramirez, O and Rapidis,
             PA and Rasmussen, L and Reucroft, S and Rijssenbeek, M and Rockwell, T and Roe, NA and Robinov, P and Ruchti, R and Rutherfoord, J and Sánchez-Hernández, A and Santoro, A and Sawyer, L and Schamberger,
             RD and Schellman, H and Sculli, J and Shabalina, E and Shaffer, C and Shankar, HC and Shivpuri, RK and Shupe, M and Singh, H and Singh, JB and Sirotenko, V and Smart, W and Smith, A and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sood, PM and Sosebee,
             M and Sotnikova, N and Souza, M and Spadafora, AL and Stephens, RW and Stevenson, ML and Stewart, D and Stoianova, DA and Stoker, D and Streets, K and Strovink, M and Sznajder, A and Tamburello, P and Tarazi,
             J and Tartaglia, M and Thomas, TLT and Thompson, J and Trippe, TG and Tuts,
             PM and Varelas, N and Varnes, EW and Vititoe, D and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, G and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Wightman, JA and Willis, S and Wimpenny, SJ and Wirjawan, JVD and Womersley, J and Won,
             E and Wood, DR and Xu, H and Yamada, R and Yamin, P and Yanagisawa, C and Yang, J and Yasuda, T and Yepes, P and Yoshikawa, C and Youssef, S and Yu,
             J and Yu, Y and Zhu, Q and Zhu, ZH and Zieminska, D and Zieminski, A and Zverev, EG and Zylberstejn, A},
   Title = {Limits on anomalous WWγ couplings from pp → Wγ + X
             events at √s = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {78},
   Number = {19},
   Pages = {3634-3639},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.78.3634},
   Abstract = {We have measured the WW? gauge boson coupling parameters
             using pp → ℓνγ + X (ℓ = e,μ) events at √s=1.8
             TeV. The data, corresponding to an integrated luminosity of
             92.8pb-1, were collected using the DØ detector at the
             Fermilab Tevatron Collider. The measured cross section times
             branching ratio for pp → Wγ+ X with pγT> 10 GeV/c and
             Rℓν> 0.7 is 11.3+1.7-1.5±1.5 pb, in agreement with the
             standard model prediction. The 1 degree of freedom 95%
             confidence level limits on individual CP-conserving
             parameters are -0.93 < Δκ < 0.94 and -0.31 < λ < 0.29.
             Similar limits are set on the CP-violating coupling
             parameters. © 1997 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.78.3634},
   Key = {Abachi97d}
}

@article{fds332359,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
             EW and Astur, R and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
             K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
             SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
             Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {Limits on anomalous [Formula Presented] and [Formula
             Presented] couplings},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {58},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.58.031102},
   Abstract = {Limits on the anomalous [Formula Presented] and [Formula
             Presented] couplings are presented from a simultaneous fit
             to the data samples of three gauge boson pair final states
             in [Formula Presented] collisions at [Formula Presented]
             [Formula Presented] production with the [Formula Presented]
             boson decaying to [Formula Presented] or μν, [Formula
             Presented] boson pair production with both of the [Formula
             Presented] bosons decaying to [Formula Presented] or μν,
             and [Formula Presented] or [Formula Presented] production
             with one [Formula Presented] boson decaying to [Formula
             Presented] and the other [Formula Presented] boson or the
             [Formula Presented] boson decaying to two jets. Assuming
             identical [Formula Presented] and [Formula Presented]
             couplings, 95% C.L. limits on the anomalous couplings of
             [Formula Presented] [Formula Presented] and [Formula
             Presented] [Formula Presented] are obtained using a form
             factor scale [Formula Presented] Limits found under other
             assumptions on the relationship between the [Formula
             Presented] and [Formula Presented] couplings are also
             presented. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.58.031102},
   Key = {fds332359}
}

@article{fds308202,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson,
             EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buescher,
             V and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum,
             Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev,
             SV and Chen, LP and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Connolly, B and Cooper,
             WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein,
             D},
   Title = {Limits on anomalous [formula presented] and [formula
             presented] couplings from [formula presented]
             production},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {62},
   Number = {5},
   Pages = {18},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.62.052005},
   Abstract = {Limits on anomalous (Formula presented) and (Formula
             presented) couplings are presented from a study of (Formula
             presented) events produced in (Formula presented) collisions
             at (Formula presented) Results from the analysis of data
             collected using the DØ detector during the 1993–1995
             Tevatron collider run at Fermilab are combined with those of
             an earlier study from the 1992–1993 run. A fit to the
             transverse momentum spectrum of the W boson yields direct
             limits on anomalous (Formula presented) and (Formula
             presented) couplings. With the assumption that the (Formula
             presented) and (Formula presented) couplings are equal, we
             obtain (Formula presented) (with (Formula presented) and
             (Formula presented) (with (Formula presented) at the 95%
             confidence level for a form-factor scale (Formula
             presented). © 2000 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.62.052005},
   Key = {fds308202}
}

@article{fds308206,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bean, A and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar,
             V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler,
             M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl,
             OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov,
             D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann,
             R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein,
             D},
   Title = {Limits on quark compositeness from high energy jets in
             [formula presented] collisions at 1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {62},
   Number = {3},
   Pages = {6},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.62.031101},
   Abstract = {Events in (Formula presented) collisions at (Formula
             presented) with total transverse energy exceeding (Formula
             presented) are used to set limits on quark substructure. The
             data are consistent with next-to-leading order QCD
             calculations. We set a lower limit of (Formula presented) at
             95% confidence on the energy scale (Formula presented) for
             compositeness in quarks, assuming a model with a left-left
             isoscalar contact interaction term. The limits on (Formula
             presented) are found to be insensitive to the sign of the
             interference term in the Lagrangian. © 2000 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.62.031101},
   Key = {fds308206}
}

@article{fds307892,
   Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams,
             DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna,
             P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M and Anduaga,
             XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R},
   Title = {Limits on the production of the standard model Higgs boson
             in pp collisions at √s=7 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {9},
   Pages = {1-30},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1728-9},
   Abstract = {A search for the Standard Model Higgs boson at the Large
             Hadron Collider (LHC) running at a centre-of-mass energy of
             7 TeV is reported, based on a total integrated luminosity of
             up to 40 pb-1 collected by the ATLAS detector in 2010.
             Several Higgs boson decay channels: H→γγ,
             H→ZZ(*)→ℓℓℓℓ, H→ZZ→ℓℓνν,
             H→ZZ→ℓℓqq, H→WW(*)→ℓνℓν and
             H→WW→ℓνqq (ℓ is e, μ) are combined in a mass range
             from 110 GeV to 600 GeV. The highest sensitivity is achieved
             in the mass range between 160 GeV and 170 GeV, where the
             expected 95% CL exclusion sensitivity is at Higgs boson
             production cross sections 2. 3 times the Standard Model
             prediction. Upper limits on the cross section for its
             production are determined. Models with a fourth generation
             of heavy leptons and quarks with Standard Model-like
             couplings to the Higgs boson are also investigated and are
             excluded at 95% CL for a Higgs boson mass in the range from
             140 GeV to 185 GeV. © 2011 CERN for the benefit of the
             ATLAS collaboration.},
   Doi = {10.1140/epjc/s10052-011-1728-9},
   Key = {fds307892}
}

@booklet{Abbott98b,
   Author = {B. Abbott and M. Abolins and B. S. Acharya and I. Adam and D. L. Adams and M. Adams and S. Ahn and H. Aihara and G. A.
             Alves and N. Amos and E. W. Anderson and R. Astur and M. M.
             Baarmand and L. Babukhadia and A. Baden and V. Balamurali and J. Balderston},
   Title = {Limits on WW gamma and WWZ couplings from W boson pair
             production},
   Journal = {Physical Review D},
   Volume = {5805},
   Number = {5},
   Pages = {art. no. -- 051101},
   Year = {1998},
   Month = {September},
   Key = {Abbott98b}
}

@booklet{Abbott97b,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
             V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt,
             A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
             M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del’signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
             M and Fatyga, MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y},
   Title = {Limits on WWZ and WWγ couplings from p¯p → ev
             jjX Events at √s=1.8TeV},
   Journal = {Physical Review Letters},
   Volume = {79},
   Number = {8},
   Pages = {1441-1446},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.1441},
   Abstract = {We present limits on anomalous WWZ and WWα couplings from a
             search for WW and WZ production in p¯p collisions at √
             s=1.8TeV. We use p¯p → ev jjX events recorded with the D0
             detector at the Fermilab Tevatron Collider during the
             1992–1995 run. The data sample corresponds to an
             integrated luminosity of 96.0±5.1pb−1. Assuming identical
             WWZ and WWα coupling parameters, the 95% C.L. limits on the
             CP−conserving couplings are −0.33 < λ < 0.36 (Δk=0)
             and −0.43 < Δk < 0.59 (λ=0), for a form factor scale =
             ⋀ 2.0TeV. Limits based on other assumptions are also
             presented. © 1997 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.79.1441},
   Key = {Abbott97b}
}

@article{fds308234,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
             EW and Astur, R and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
             K and De, K and Signore, KD and Demarteau, M and Denisov, D and Denisov,
             SP and Diehl, HT and Diesburg, M and Loreto, GD and Draper, P and Ducros,
             Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Gavrilov, V and Geld, TL and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gibbard, B and Glenn, S and Gobbi, B and Goldschmidt, A and Gómez, B and Gómez, G and Goncharov,
             PI and Solís, JLG and Gordon, H and Goss, LT and Gounder, K and Goussiou,
             A and Graf, N and Grannis, PD and Green, DR and Greenlee, H and Grinstein,
             S and Grudberg, P and Grünendahl, S and Guglielmo, G and Guida, JA and Guida, JM and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez,
             P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn,
             KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hedin, D and Heinson, AP and Heintz, U and Hernández-Montoya, R and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hsieh, F and Ting, H and Tong, H and Huehn, T and Ito, AS and James, E and Jaques, J and Jerger, SA and Jesik, R and Jiang, JZY and Joffe-Minor, T and Johari, H and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Jun, SY and Jung, CK and Kahn, S and Kalbfleisch, G and Kang, JS and Karmanov, D and Karmgard, D and Kehoe, R and Kelly, ML and Kim, CL and Kim,
             SK and Klima, B and Klopfenstein, C and Kohli, JM and Koltick, D and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kourlas, J and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kuleshov, S and Kunori, S and Landry, F and Landsberg, G and Lauer, B and Leflat, A and Li, H and Li, J and Li-Demarteau, QZ and Lima, JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Liu, YC and Lobkowicz, F and Loken, SC and Lökös, S and Lueking, L and Lyon, AL and Maciel, AKA and Madaras, RJ and Madden, R and Magaña-Mendoza, L and Manankov, V and Mani, S and Mao,
             HS and Markeloff, R and Marshall, T and Martin, MI and Mauritz, KM and May,
             B and Mayorov, AA and McCarthy, R and McDonald, J and McKibben, T and McKinley, J and McMahon, T and Melanson, HL and Merkin, M and Merritt,
             KW and Miettinen, H and Mincer, A and Mishra, CS and Mokhov, N and Mondal,
             NK and Montgomery, HE and Mooney, P and Motta, HD and Murphy, C and Nang,
             F and Narain, M and Narasimham, VS and Narayanan, A and Neal, HA and Negret, JP and Nemethy, P and Norman, D and Oesch, L and Oguri, V and Oliveira, E and Oltman, E and Oshima, N and Owen, D and Padley, P and Para,
             A and Park, YM and Partridge, R and Parua, N and Paterno, M and Pawlik, B and Perkins, J and Peters, M and Piegaia, R and Piekarz, H and Pischalnikov,
             Y and Pope, BG and Prosper, HB and Protopopescu, S and Qian, J and Quintas,
             PZ and Raja, R and Rajagopalan, S and Ramirez, O and Rasmussen, L and Reucroft, S and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov,
             P and Ruchti, R and Rutherfoord, J and Sánchez-Hernández, A and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Sculli, J and Shabalina, E and Shaffer, C and Shankar, HC and Shivpuri,
             RK and Shupe, M and Singh, H and Singh, JB and Sirotenko, V and Smart, W and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder,
             S and Solomon, J and Sosebee, M and Sotnikova, N and Souza, M and Spadafora, AL and Steinbrück, G and Stephens, RW and Stevenson, ML and Stewart, D and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova,
             DA and Strauss, M and Streets, K and Strovink, M and Sznajder, A and Tamburello, P and Tarazi, J and Tartaglia, M and Thomas, TLT and Thompson, J and Trippe, TG and Tuts, PM and Varelas, N and Varnes, EW and Vititoe, D and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, G and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White,
             JT and Wightman, JA and Willis, S and Wimpenny, SJ and Wirjawan, JVD and Womersley, J and Won, E and Wood, DR and Xu, H and Yamada, R and Yamin, P and Yang, J and Yasuda, T and Yepes, P and Yoshikawa, C and Youssef, S and Yu,
             J and Yu, Y and Zhou, Z and Zhu, ZH and Zieminska, D and Zieminski, A and Zverev, EG and Zylberstejn, A},
   Title = {Limits on WWγ and WWZ couplings from IV boson pair
             production},
   Journal = {Physical Review D},
   Volume = {58},
   Number = {5},
   Pages = {DUMMY1},
   Year = {1998},
   Abstract = {The results of a search for W boson pair production in pp
             collisions at √s= 1.8 TeV with subsequent decay to eμ,
             ee, and μμ channels are presented. Five candidate events
             are observed with an expected background of 3.1 ±0.4 events
             for an integrated luminosity of approximately 97 pb-1.
             Limits on the anomalous couplings are obtained from a
             maximum likelihood fit of the ET spectra of the leptons in
             the candidate events. Assuming identical WWγ and WWZ
             couplings, the 95% C.L. limits are -0.62&lt;Δκ&lt;0.77 (X.
             = 0) and -0.53&lt;λ &lt;0.56 (Δκ=0) for a form factor
             scale Λ= 1.5 TeV. © 1998 The American Physical
             Society.},
   Key = {fds308234}
}

@article{fds308233,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
             EW and Astur, R and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
             K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
             SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
             Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {Limits on [Formula Presented] and [Formula Presented]
             couplings from [Formula Presented] boson pair
             production},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {58},
   Number = {5},
   Pages = {511011-511016},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   ISSN = {0556-2821},
   url = {http://dx.doi.org/10.1103/PhysRevD.58.051101},
   Abstract = {The results of a search for [Formula Presented] boson pair
             production in [Formula Presented] collisions at [Formula
             Presented] with subsequent decay to [Formula Presented]
             [Formula Presented] and μμ channels are presented. Five
             candidate events are observed with an expected background of
             [Formula Presented] events for an integrated luminosity of
             approximately [Formula Presented] Limits on the anomalous
             couplings are obtained from a maximum likelihood fit of the
             [Formula Presented] spectra of the leptons in the candidate
             events. Assuming identical [Formula Presented] and [Formula
             Presented] couplings, the 95% C.L. limits are [Formula
             Presented] [Formula Presented] and [Formula Presented]
             [Formula Presented] [Formula Presented] for a form factor
             scale [Formula Presented]. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.58.051101},
   Key = {fds308233}
}

@article{fds356026,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei,
             V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo
             Pereira, R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin,
             J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Artz, S and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Avolio, G and Ayoub, MK and Azuelos, G and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis,
             C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
             E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak,
             L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
             P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
             A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertram, IA and Bessidskaia Bylund and O and Besson,
             N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya, DS and Bhattarai, P and Bi, R and Bianchi, RM and Biebel,
             O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
             JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner,
             R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko,
             D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burr, JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba,
             LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carter, JWS and Casado, MP and Casha,
             AF and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavallaro, E and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Cerda Alberich and L and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen,
             SJ and Chen, X and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Chytka, L and Cieri, D and Ciesla, KM and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio,
             M},
   Title = {Longitudinal Flow Decorrelations in Xe+Xe Collisions at
             sqrt[s_{NN}]=5.44  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {126},
   Number = {12},
   Pages = {122301},
   Year = {2021},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.126.122301},
   Abstract = {The first measurement of longitudinal decorrelations of
             harmonic flow amplitudes v_{n} for n=2-4 in Xe+Xe collisions
             at sqrt[s_{NN}]=5.44  TeV is obtained using
             3  μb^{-1} of data with the ATLAS detector at the LHC.
             The decorrelation signal for v_{3} and v_{4} is found to be
             nearly independent of collision centrality and transverse
             momentum (p_{T}) requirements on final-state particles, but
             for v_{2} a strong centrality and p_{T} dependence is seen.
             When compared with the results from Pb+Pb collisions at
             sqrt[s_{NN}]=5.02  TeV, the longitudinal decorrelation
             signal in midcentral Xe+Xe collisions is found to be larger
             for v_{2}, but smaller for v_{3}. Current hydrodynamic
             models reproduce the ratios of the v_{n} measured in Xe+Xe
             collisions to those in Pb+Pb collisions but fail to describe
             the magnitudes and trends of the ratios of longitudinal flow
             decorrelations between Xe+Xe and Pb+Pb. The results on the
             system-size dependence provide new insights and an important
             lever arm to separate effects of the longitudinal structure
             of the initial state from other early and late time effects
             in heavy-ion collisions.},
   Doi = {10.1103/physrevlett.126.122301},
   Key = {fds356026}
}

@article{fds321073,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
             N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
             F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
             EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
             R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo,
             F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez,
             VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Luminosity determination in pp collisions at [Formula: see
             text] = 8 TeV using the ATLAS detector at the
             LHC.},
   Journal = {Eur Phys J C Part Fields},
   Volume = {76},
   Number = {12},
   Pages = {653},
   Year = {2016},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4466-1},
   Abstract = {The luminosity determination for the ATLAS detector at the
             LHC during pp collisions at [Formula: see text] 8 TeV in
             2012 is presented. The evaluation of the luminosity scale is
             performed using several luminometers, and comparisons
             between these luminosity detectors are made to assess the
             accuracy, consistency and long-term stability of the
             results. A luminosity uncertainty of [Formula: see text] is
             obtained for the [Formula: see text] of pp collision data
             delivered to ATLAS at [Formula: see text] 8 TeV in
             2012.},
   Doi = {10.1140/epjc/s10052-016-4466-1},
   Key = {fds321073}
}

@article{fds373905,
   Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
             BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
             W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
             AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung,
             C and Amerl, M and Ames, CG and Amidei, D and Dos Santos and SPA and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH},
   Title = {Luminosity determination in pp collisions at √s=13 TeV
             using the ATLAS detector at the LHC},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {10},
   Year = {2023},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11747-w},
   Abstract = {The luminosity determination for the ATLAS detector at the
             LHC during Run 2 is presented, with pp collisions at a
             centre-of-mass energy s=13 TeV. The absolute luminosity
             scale is determined using van der Meer beam separation scans
             during dedicated running periods in each year, and
             extrapolated to the physics data-taking regime using
             complementary measurements from several luminosity-sensitive
             detectors. The total uncertainties in the integrated
             luminosity for each individual year of data-taking range
             from 0.9% to 1.1%, and are partially correlated between
             years. After standard data-quality selections, the full
             Run 2 pp data sample corresponds to an integrated
             luminosity of 140.1 ± 1.2 fb - 1 , i.e. an uncertainty of
             0.83%. A dedicated sample of low-pileup data recorded in
             2017–2018 for precision Standard Model physics
             measurements is analysed separately, and has an integrated
             luminosity of 338.1 ± 3.1 pb - 1 .},
   Doi = {10.1140/epjc/s10052-023-11747-w},
   Key = {fds373905}
}

@article{fds310263,
   Author = {Hinchliffe, I and Kotwal, A and Mangano, ML and Quigg, C and Wang,
             LT},
   Title = {Luminosity goals for a 100-TeV pp collider},
   Journal = {International Journal of Modern Physics A},
   Volume = {30},
   Number = {23},
   Pages = {1544002-1544002},
   Publisher = {World Scientific Pub Co Pte Lt},
   Year = {2015},
   Month = {August},
   ISSN = {0217-751X},
   url = {http://dx.doi.org/10.1142/S0217751X15440029},
   Abstract = {We consider diverse examples of science goals that provide a
             framework to assess luminosity goals for a future 100-TeV
             proton-proton collider.},
   Doi = {10.1142/S0217751X15440029},
   Key = {fds310263}
}

@article{fds227090,
   Author = {Ian Hinchliffe and Ashutosh Kotwal and Michelangelo L. Mangano and Chris Quigg and Lian-Tao Wang},
   Title = {Luminosity goals for a 100-TeV pp collider},
   Journal = {Int.J.Mod.Phys. A},
   Volume = {30},
   Number = {1544002},
   Year = {2015},
   Month = {April},
   Key = {fds227090}
}

@article{fds307539,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Mass and lifetime measurements of bottom and charm baryons
             in p p ̄ collisions at s =1.96TeV MASS and LIFETIME
             MEASUREMENTS of BOTTOM and ⋯ T. AALTONEN},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {April},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.072014},
   Abstract = {We report on mass and lifetime measurements of several
             ground state charmed and bottom baryons, using a data sample
             corresponding to 9.6fb-1 from pp̄ collisions at s=1.96TeV
             and recorded with the Collider Detector at Fermilab. Baryon
             candidates are reconstructed from data collected with an
             online event selection designed for the collection of
             long-lifetime heavy-flavor decay products and a second event
             selection designed to collect J/ ψ→μ+μ- candidates.
             First evidence for the process Ωb-→Ωc0π- is presented
             with a significance of 3.3σ. We measure the following
             baryon masses: M(Ξc0)=2470.85±0.24(stat)
             ±0.55(syst)MeV/c2,M(Ξc+)=2468.00±0.18(stat)±0.51(syst)
             MeV/c2,M(Λb)=5620.15±0.31(stat)±0.47(syst)MeV/c2,M(Ξb-)=
             5793.4±1.8(stat)±0.7(syst)MeV/c2,M(Ξb0)=5788.7±4.3(stat)
             ±1.4(syst)MeV/c2,andM(Ωb-)=6047.5±3.8(stat)±0.6(syst)
             MeV/c2.The isospin splitting of the Ξb-,0 states is found
             to be M(Ξb-)-M(Ξb0)=4.7±4.7(stat)±0.7(syst)MeV/c2. The
             isospin splitting of the Ξc0,+ states is found to be
             M(Ξc0)-M(Ξc+)=2. 85±0.30(stat)±0.04(syst)MeV/c2. The
             following lifetime measurements are made:
             τ(Λb)=1.565±0.035(stat)±0. 020(syst)ps,τ(Ξb-)=1.32±0.14(stat)±0.02(syst)ps,
             τ(Ωb-)=1.66-0.40+0.53(stat)±0.02(syst)ps. © 2014
             American Physical Society.},
   Doi = {10.1103/PhysRevD.89.072014},
   Key = {fds307539}
}

@article{fds346185,
   Author = {Agrawal, S and Puthia, A and Kotwal, A and Tilak, R and Kunte, R and Kushwaha, AS},
   Title = {Mass scabies management in an orphanage of rural community:
             An experience.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {68},
   Number = {4},
   Pages = {403-406},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.mjafi.2012.02.014},
   Doi = {10.1016/j.mjafi.2012.02.014},
   Key = {fds346185}
}

@article{fds308096,
   Author = {Acosta, and D, and others},
   Title = {Measurement of $b$ hadron masses in exclusive $J/\psi$
             decays with the CDF detector},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {20},
   Pages = {202001},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.202001},
   Abstract = {We measure the masses of $b$ hadrons in exclusively
             reconstructed final states containing a $J/\psi\to\mu^-\mu^+$
             decay using $\rm 220 pb^{-1}$ of data collected by the CDF
             II experiment. We find: m(B^+) = 5279.10 \pm 0.41_{(stat.)}
             \pm 0.36_{(sys.)} MeVcc, m(B^0) = 5279.63 \pm 0.53_{(stat.)}
             \pm 0.33_{(sys.)} MeVcc, m(B^0_s) = 5366.01 \pm
             0.73_{(stat.)} \pm 0.33_{(sys.)} MeVcc, m(\Lambda^0_b) =
             5619.7 \pm 1.2_{(stat.)} \pm 1.2_{(sys.)} MeVcc. m(B^+) -
             m(B^0) = -0.53 \pm 0.67_{(stat.)} \pm 0.14_{(sys.)} MeVcc,
             m(B^0_s) - m(B^0) = 86.38 \pm 0.90_{(stat.)} \pm
             0.06_{(sys.)} MeVcc m(\Lambda^0_b) - m(B^0) = 339.2 \pm
             1.4_{(stat.)} \pm 0.1_{(sys.)} MeVcc. The measurements of
             the $B^0_s$, $\Lambda^0_b$ mass, $m(B^0_s)-m(B^0)$ and
             $m(\Lambda^0_b)-m(B^0)$ mass difference are of better
             precision than the current world averages.},
   Doi = {10.1103/physrevlett.96.202001},
   Key = {fds308096}
}

@article{fds307877,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of $t\overline{t}$ spin correlation in
             $p\overline{p}$ collisions using the CDF II detector at the
             Tevatron},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {3},
   Pages = {031104},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.031104},
   Abstract = {The tt̄ spin correlation at production is a fundamental
             prediction of QCD and a potentially incisive test of new
             physics coupled to top quarks. We measure the tt̄ spin
             state in pp̄ collisions at √s=1.96TeV using 1001
             candidate events in the lepton plus jets decay channel
             reconstructed in the CDF II detector. In the helicity basis,
             for a top-quark mass of 172.5GeV/c2, we find a spin
             correlation coefficient κ=0.60±0.50(stat)±0. 16(syst),
             consistent with the QCD prediction, κ 0.40. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.83.031104},
   Key = {fds307877}
}

@article{fds307920,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of $Z\gamma{}$ production in $pp[over
             \ifmmode\bar\else\textasciimacron\fi{}]$ collisions at
             $\sqrt{s}=1.96\,\,TeV$},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {3},
   Pages = {031103},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.031103},
   Abstract = {The production rate and kinematics of photons produced in
             association with Z bosons are studied using 2fb-1 of pp̄
             collision data collected at the Collider Detector at
             Fermilab. The cross section for pp̄→"+-γ+X (where the
             leptons " are either muons or electrons with dilepton mass
             M>40GeV/c2, and where the photon has transverse energy
             ETγ>7GeV and is well separated from the leptons) is
             4.6±0.2(stat)±0.3(syst)±0.3(lum)pb, which is consistent
             with standard model expectations. We use the photon ET
             distribution from Zγ events where the Z has decayed to
             μ+μ -, e+e-, or νν̄ to set limits on anomalous (non
             standard model) trilinear couplings between photons and Z
             bosons. © 2010 The American Physical Society.},
   Doi = {10.1103/PhysRevD.82.031103},
   Key = {fds307920}
}

@article{fds307852,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of ${b}$ Hadron Lifetimes in Exclusive Decays
             Containing a ${J}/\psi$ in $p\overline{p}$ Collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {12},
   Pages = {121804},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.121804},
   Abstract = {We report on a measurement of b-hadron lifetimes in the
             fully reconstructed decay modes B(+)→J/ψK(+),
             B⁰→J/ψK*(892)⁰, B⁰→J/ψK(s)⁰, and
             Λ(b)⁰→J/ψΛ⁰ using data corresponding to an
             integrated luminosity of 4.3 fb⁻¹, collected by the CDF
             II detector at the Fermilab Tevatron. The measured lifetimes
             are τ(B(+))=[1.639±0.009(stat)±0.009(syst)] ps,
             τ(B⁰)=[1.507±0.010(stat)±0.008(syst)] ps, and
             τ(Λ(b)⁰)=[1.537±0.045(stat)±0.014(syst)] ps. The
             lifetime ratios are τ(B(+))/τ(B⁰)=[1.088±0.009(stat)±0.004(syst)]
             and τ(Λ(b)⁰)/τ(B⁰)=[1.020±0.030(stat)±0.008(syst)].
             These are the most precise determinations of these
             quantities from a single experiment.},
   Doi = {10.1103/PhysRevLett.106.121804},
   Key = {fds307852}
}

@article{fds307604,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Auerbach,
             B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli,
             F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behar Harpaz and S and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt,
             J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda,
             V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C},
   Title = {Measurement of kT splitting scales in
             Wℓν events at [Formula: see text] with
             the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {5},
   Pages = {2432},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2432-8},
   Abstract = {A measurement of splitting scales, as defined by the
             <i>k</i><sub>T</sub> clustering algorithm, is presented for
             final states containing a <i>W</i> boson produced in
             proton-proton collisions at a centre-of-mass energy of
             7 TeV. The measurement is based on the full 2010 data
             sample corresponding to an integrated luminosity of
             36 pb<sup>-1</sup> which was collected using the ATLAS
             detector at the CERN Large Hadron Collider. Cluster
             splitting scales are measured in events containing <i>W</i>
             bosons decaying to electrons or muons. The measurement
             comprises the four hardest splitting scales in a
             <i>k</i><sub>T</sub> cluster sequence of the hadronic
             activity accompanying the <i>W</i> boson, and ratios of
             these splitting scales. Backgrounds such as multi-jet and
             top-quark-pair production are subtracted and the results are
             corrected for detector effects. Predictions from various
             Monte Carlo event generators at particle level are compared
             to the data. Overall, reasonable agreement is found with all
             generators, but larger deviations between the predictions
             and the data are evident in the soft regions of the
             splitting scales.},
   Doi = {10.1140/epjc/s10052-013-2432-8},
   Key = {fds307604}
}

@article{fds307770,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi,
             E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
             J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
             PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas,
             CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
             X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W},
   Title = {Measurement of τ polarization in
             Wτν decays with the ATLAS detector in
             pp collisions at [Formula: see text].},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {72},
   Number = {7},
   Pages = {2062},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2062-6},
   Abstract = {In this paper, a measurement of <i>τ</i> polarization in
             <i>W</i>→<i>τν</i> decays is presented. It is measured
             from the energies of the decay products in hadronic
             <i>τ</i> decays with a single final state charged particle.
             The data, corresponding to an integrated luminosity of
             24 pb<sup>-1</sup>, were collected by the ATLAS experiment
             at the Large Hadron Collider in 2010. The measured value of
             the <i>τ</i> polarization is [Formula: see text], in
             agreement with the Standard Model prediction, and is
             consistent with a physically allowed 95 % CL
             interval [-1,-0.91]. Measurements of <i>τ</i> polarization
             have not previously been made at hadron colliders.},
   Doi = {10.1140/epjc/s10052-012-2062-6},
   Key = {fds307770}
}

@article{fds356554,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
             Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V},
   Title = {Measurement of angular and momentum distributions of charged
             particles within and around jets in Pb+Pb and pp collisions
             at sNN =5.02 TeV with the ATLAS detector},
   Journal = {Physical Review C},
   Volume = {100},
   Number = {6},
   Year = {2019},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevC.100.064901},
   Abstract = {Studies of the fragmentation of jets into charged particles
             in heavy-ion collisions can provide information about the
             mechanism of jet quenching by the hot and dense QCD matter
             created in such collisions, the quark-gluon plasma. This
             paper presents a measurement of the angular distribution of
             charged particles around the jet axis in sNN=5.02 TeV Pb+Pb
             and pp collisions, using the ATLAS detector at the LHC. The
             Pb+Pb and pp data sets have integrated luminosities of
             0.49nb-1 and 25pb-1, respectively. The measurement is
             performed for jets reconstructed with the anti-kt algorithm
             with radius parameter R=0.4 and is extended to an angular
             distance of r=0.8 from the jet axis. Results are presented
             as a function of Pb+Pb collision centrality and distance
             from the jet axis for charged particles with transverse
             momenta in the 1- to 63-GeV range, matched to jets with
             transverse momenta in the 126- to 316-GeV range and an
             absolute value of jet rapidity of less than 1.7.
             Modifications to the measured distributions are quantified
             by taking a ratio to the measurements in pp collisions.
             Yields of charged particles with transverse momenta below 4
             GeV are observed to be increasingly enhanced as a function
             of angular distance from the jet axis, reaching a maximum at
             r=0.6. Charged particles with transverse momenta above 4 GeV
             have an enhanced yield in Pb+Pb collisions in the jet core
             for angular distances up to r=0.05 from the jet axis, with a
             suppression at larger distances.},
   Doi = {10.1103/PhysRevC.100.064901},
   Key = {fds356554}
}

@article{fds307611,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Measurement of angular correlations in Drell–Yan lepton
             pairs to probe Z/γ boson transverse momentum
             at √s=7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {720},
   Number = {1-3},
   Pages = {32-51},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.054},
   Abstract = {A measurement of angular correlations in Drell–Yan lepton
             pairs via the ϕη⁎ observable is presented. This variable
             probes the same physics as the Z/γ⁎ boson transverse
             momentum with a better experimental resolution. The
             Z/γ⁎→e+e− and Z/γ⁎→μ+μ− decays produced in
             proton–proton collisions at a centre-of-mass energy of
             sqrts=7 TeV are used. The data were collected with the ATLAS
             detector at the LHC and correspond to an integrated
             luminosity of 4.6 fb−1. Normalised differential cross
             sections as a function of ϕη⁎ are measured separately
             for electron and muon decay channels. These channels are
             then combined for improved accuracy. The cross section is
             also measured double differentially as a function of ϕη⁎
             for three independent bins of the Z boson rapidity. The
             results are compared to QCD calculations and to predictions
             from different Monte Carlo event generators. The data are
             reasonably well described, in all measured Z boson rapidity
             regions, by resummed QCD predictions combined with
             fixed-order perturbative QCD calculations or by some Monte
             Carlo event generators. The measurement precision is
             typically better by one order of magnitude than present
             theoretical uncertainties.},
   Doi = {10.1016/j.physletb.2013.01.054},
   Key = {fds307611}
}

@article{fds351087,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei,
             V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo
             Pereira, R},
   Title = {Measurement of azimuthal anisotropy of muons from charm and
             bottom hadrons in Pb+Pb collisions at sNN=5.02
             TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {807},
   Year = {2020},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2020.135595},
   Abstract = {Azimuthal anisotropies of muons from charm and bottom hadron
             decays are measured in Pb+Pb collisions at sNN=5.02TeV. The
             data were collected with the ATLAS detector at the Large
             Hadron Collider in 2015 and 2018 with integrated
             luminosities of 0.5nb−1 and 1.4nb−1, respectively. The
             kinematic selection for heavy-flavor muons requires
             transverse momentum 4<pT<30GeV and pseudorapidity |η|<2.0.
             The dominant sources of muons in this pT range are
             semi-leptonic decays of charm and bottom hadrons. These
             heavy-flavor muons are separated from light-hadron decay
             muons and punch-through hadrons using the momentum imbalance
             between the measurements in the tracking detector and in the
             muon spectrometers. Azimuthal anisotropies, quantified by
             flow coefficients, are measured via the event-plane method
             for inclusive heavy-flavor muons as a function of the muon
             pT and in intervals of Pb+Pb collision centrality.
             Heavy-flavor muons are separated into contributions from
             charm and bottom hadron decays using the muon transverse
             impact parameter with respect to the event primary vertex.
             Non-zero elliptic (v2) and triangular (v3) flow coefficients
             are extracted for charm and bottom muons, with the charm
             muon coefficients larger than those for bottom muons for all
             Pb+Pb collision centralities. The results indicate
             substantial modification to the charm and bottom quark
             angular distributions through interactions in the
             quark-gluon plasma produced in these Pb+Pb collisions, with
             smaller modifications for the bottom quarks as expected
             theoretically due to their larger mass.},
   Doi = {10.1016/j.physletb.2020.135595},
   Key = {fds351087}
}

@article{fds348980,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
             Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling,
             J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assahsah,
             J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay,
             NB and Atmani, H and Augsten, K and Avolio, G and Avramidou, R and Ayoub,
             MK and Azoulay, AM and Azuelos, G and Bachacou, H and Bachas, K and Backes,
             M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin,
             EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour,
             G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barsov, S and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertram, IA and Bessidskaia Bylund and O and Besson, N and Bethani,
             A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya,
             DS and Bhattarai, P and Bi, R and Bianchi, RM and Biebel, O and Biedermann,
             D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borecka-Bielska, HM and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
             DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
             G and Brooks, WK and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton,
             CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carter, JWS and Casado, MP and Casha, AF and Casper, DW and Castelijn,
             R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, SK and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen,
             Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias,
             TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Chu,
             MC},
   Title = {Measurement of Azimuthal Anisotropy of Muons from Charm and
             Bottom Hadrons in pp Collisions at sqrt[s]=13  TeV with
             the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {124},
   Number = {8},
   Pages = {082301},
   Year = {2020},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.124.082301},
   Abstract = {The elliptic flow of muons from the decay of charm and
             bottom hadrons is measured in pp collisions at
             sqrt[s]=13  TeV using a data sample with an integrated
             luminosity of 150  pb^{-1} recorded by the ATLAS
             detector at the LHC. The muons from heavy-flavor decay are
             separated from light-hadron decay muons using momentum
             imbalance between the tracking and muon spectrometers. The
             heavy-flavor decay muons are further separated into those
             from charm decay and those from bottom decay using the
             distance-of-closest-approach to the collision vertex. The
             measurement is performed for muons in the transverse
             momentum range 4-7 GeV and pseudorapidity range |η|<2.4. A
             significant nonzero elliptic anisotropy coefficient v_{2} is
             observed for muons from charm decays, while the v_{2} value
             for muons from bottom decays is consistent with zero within
             uncertainties.},
   Doi = {10.1103/physrevlett.124.082301},
   Key = {fds348980}
}

@article{fds351560,
   Author = {Acosta, and D, and others},
   Title = {Measurement of B(t --> W b)/B(t --> W q) at the Collider
             Detector at Fermilab},
   Journal = {Phys. Rev. Lett.},
   Volume = {95},
   Number = {10},
   Pages = {102002},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/physrevlett.95.102002},
   Abstract = {http://arxiv.org/abs/hep-ex/0505091},
   Doi = {10.1103/physrevlett.95.102002},
   Key = {fds351560}
}

@article{fds310396,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
             JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
             A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
             C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
             L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and (CDF
             Collaboration)},
   Title = {Measurement of B(t→Wb)/B(t→Wq) in top-quark-pair decays
             using dilepton events and the full CDF Run II data
             set.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {22},
   Pages = {221801},
   Year = {2014},
   Month = {June},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.112.221801},
   Abstract = {We present a measurement of the ratio of the top-quark
             branching fractions R=B(t→Wb)/B(t→Wq), where q
             represents any quark flavor, in events with two charged
             leptons, imbalance in total transverse energy, and at least
             two jets. The measurement uses proton-antiproton collision
             data at center-of-mass energy 1.96 TeV, corresponding to an
             integrated luminosity of 8.7  fb^{-1} collected with the
             Collider Detector at Fermilab during Run II of the Tevatron.
             We measure R to be 0.87±0.07, and extract the magnitude of
             the top-bottom quark coupling to be |V_{tb}|=0.93±0.04,
             assuming three generations of quarks. Under these
             assumptions, a lower limit of |V_{tb}|>0.85(0.87) at 95%
             (90%) credibility level is set.},
   Doi = {10.1103/physrevlett.112.221801},
   Key = {fds310396}
}

@article{fds356725,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Measurement of b-hadron pair production with the ATLAS
             detector in proton-proton collisions at √s=8
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {11},
   Year = {2017},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2017)062},
   Abstract = {A measurement of b-hadron pair production is presented,
             based on a data set corresponding to an integrated
             luminosity of 11.4 fb−1 of proton-proton collisions
             recorded at s=8 TeV with the ATLAS detector at the LHC.
             Events are selected in which a b-hadron is reconstructed in
             a decay channel containing J/ψ → μμ, and a second
             b-hadron is reconstructed in a decay channel containing a
             muon. Results are presented in a fiducial volume defined by
             kinematic requirements on three muons based on those used in
             the analysis. The fiducial cross section is measured to be
             17.7 ± 0.1(stat.) ± 2.0(syst.) nb. A number of normalised
             differential cross sections are also measured, and compared
             to predictions from the Pythia8, Herwig++,
             MadGraph5_aMC@NLO+Pythia8 and Sherpa event generators,
             providing new constraints on heavy flavour
             production.[Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP11(2017)062},
   Key = {fds356725}
}

@article{fds361168,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S},
   Title = {Measurement of b-quark fragmentation properties in jets
             using the decay B ± → J/ψK ± in
             pp collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {12},
   Year = {2021},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2021)131},
   Abstract = {The fragmentation properties of jets containing b-hadrons
             are studied using charged B mesons in 139 fb−1 of pp
             collisions at s = 13 TeV, recorded with the ATLAS detector
             at the LHC during the period from 2015 to 2018. The B mesons
             are reconstructed using the decay of B± into J/ψK±, with
             the J/ψ decaying into a pair of muons. Jets are
             reconstructed using the anti-kt algorithm with radius
             parameter R = 0.4. The measurement determines the
             longitudinal and transverse momentum profiles of the
             reconstructed B hadrons with respect to the axes of the jets
             to which they are geometrically associated. These
             distributions are measured in intervals of the jet
             transverse momentum, ranging from 50 GeV to above 100 GeV.
             The results are corrected for detector effects and compared
             with several Monte Carlo predictions using different parton
             shower and hadronisation models. The results for the
             longitudinal and transverse profiles provide useful inputs
             to improve the description of heavy-flavour fragmentation in
             jets. [Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP12(2021)131},
   Key = {fds361168}
}

@article{fds307886,
   Author = {Aaltonen, TEA},
   Title = {Measurement of branching ratio and ${B}_{s}^{0}$ lifetime in
             the decay ${B}_{s}^{0}\rightarrow{J}/\psi{f}_{0}(980)$ at
             {CDF}},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {5},
   Pages = {052012},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.052012},
   Abstract = {We present a study of Bs0 decays to the CP-odd final state
             J/ψf 0(980) with J/ψ→μ+μ- and f 0(980)→π+π-. Using
             pp̄ collision data with an integrated luminosity of 3.8fb-1
             collected by the CDF II detector at the Tevatron we measure
             a Bs0 lifetime of τ(Bs0→J/ψf0(980))=1.70-0.11+0.12(stat)±0.03(syst)
             ps. This is the first measurement of the Bs0 lifetime in a
             decay to a CP eigenstate and corresponds in the standard
             model to the lifetime of the heavy Bs0 eigenstate. We also
             measure the product of branching fractions of
             Bs0→J/ψf0(980) and f0(980)→π +π- relative to the
             product of branching fractions of Bs0→J/ψ and →K+K- to
             be Rf0 /=0.257±0.020(stat)±0.014(syst), which is the most
             precise determination of this quantity to date. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.84.052012},
   Key = {fds307886}
}

@article{fds307705,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of Bs0→Ds(*)+Ds(*)- branching
             ratios.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {20},
   Pages = {201801},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.201801},
   Abstract = {The decays Bs0→Ds(*)+Ds(*)- are reconstructed in a data
             sample corresponding to an integrated luminosity of
             6.8  fb-1 collected by the CDF II detector at the
             Tevatron pp[over ¯] collider. All decay modes are observed
             with a significance of more than 10σ, and we measure the
             Bs0 production rate times Bs0→Ds(*)+Ds(*)- branching
             ratios relative to the normalization mode B0→Ds+D-to be
             0.183±0.021±0.017 for Bs0→Ds+Ds-, 0.424±0.046±0.035
             for Bs0→Ds*±Ds^∓, 0.654±0.072±0.065 for
             Bs0→Ds*+Ds*-, and 1.261±0.095±0.112 for the inclusive
             decay Bs0→Ds(*)+Ds(*)-, where the uncertainties are
             statistical and systematic. These results are the most
             precise single measurements to date and provide important
             constraints for indirect searches for nonstandard model
             physics in Bs0 mixing.},
   Doi = {10.1103/physrevlett.108.201801},
   Key = {fds307705}
}

@article{fds310287,
   Author = {Aaltonen, T and Albrow, MG and Amerio, S and Amidei, D and Anastassov,
             A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
             T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri,
             A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
             B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
             A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
             F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
             DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
             B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher,
             R},
   Title = {Measurement of central exclusive π+π- production in p p ¯
             collisions at s =0.9 and 1.96 TeV at CDF MEASUREMENT of
             CENTRAL EXCLUSIVE π+π- ... T. AALTONEN et
             al.},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.091101},
   Abstract = {We measure exclusive π+π- production in proton-antiproton
             collisions at center-of-mass energies s=0.9 and 1.96 TeV in
             the Collider Detector at Fermilab. We select events with two
             oppositely charged particles, assumed to be pions, with
             pseudorapidity |η|<1.3 and with no other particles detected
             in |η|<5.9. We require the π+π- system to have rapidity
             |y|<1.0. The production mechanism of these events is
             expected to be dominated by double pomeron exchange, which
             constrains the quantum numbers of the central state. The
             data are potentially valuable for isoscalar meson
             spectroscopy and for understanding the pomeron in a region
             of transition between nonperturbative and perturbative
             quantum chromodynamics. The data extend up to dipion mass
             M(π+π-)=5000MeV/c2 and show resonance structures
             attributed to f0 and f2(1270) mesons. From the π+π- and
             K+K- spectra, we place upper limits on exclusive χc0(3415)
             production.},
   Doi = {10.1103/PhysRevD.91.091101},
   Key = {fds310287}
}

@article{fds356758,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
             M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
             D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Measurement of charged-particle distributions sensitive to
             the underlying event in √s=13 TeV proton-proton collisions
             with the ATLAS detector at the LHC},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {3},
   Year = {2017},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2017)157},
   Abstract = {We present charged-particle distributions sensitive to the
             underlying event, measured by the ATLAS detector in
             proton-proton collisions at a centre-of-mass energy of 13
             TeV, in low-luminosity Large Hadron Collider fills
             corresponding to an integrated luminosity of 1.6 nb−1. The
             distributions were constructed using charged particles with
             absolute pseudorapidity less than 2.5 and with transverse
             momentum greater than 500 MeV, in events with at least one
             such charged particle with transverse momentum above 1 GeV.
             These distributions characterise the angular distribution of
             energy and particle flows with respect to the charged
             particle with highest transverse momentum, as a function of
             both that momentum and of charged-particle multiplicity. The
             results have been corrected for detector effects and are
             compared to the predictions of various Monte Carlo event
             generators, experimentally establishing the level of
             underlying-event activity at LHC Run 2 energies and
             providing inputs for the development of event generator
             modelling. The current models in use for UE modelling
             typically describe this data to 5% accuracy, compared with
             data uncertainties of less than 1%.[Figure not available:
             see fulltext.]},
   Doi = {10.1007/JHEP03(2017)157},
   Key = {fds356758}
}

@article{fds307586,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Measurement of charged-particle event shape variables in
             inclusive √(s)=7 TeV proton-proton interactions with the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.032004},
   Abstract = {The measurement of charged-particle event shape variables is
             presented in inclusive inelastic pp collisions at a
             center-of-mass energy of 7 TeV using the ATLAS detector at
             the LHC. The observables studied are the transverse thrust,
             thrust minor, and transverse sphericity, each defined using
             the final-state charged particles' momentum components
             perpendicular to the beam direction. Events with at least
             six charged particles are selected by a minimum-bias
             trigger. In addition to the differential distributions, the
             evolution of each event shape variable as a function of the
             leading charged-particle transverse momentum,
             charged-particle multiplicity, and summed transverse
             momentum is presented. Predictions from several Monte Carlo
             models show significant deviations from data. © 2013 CERN.
             Published by the American Physical Society.},
   Doi = {10.1103/PhysRevD.88.032004},
   Key = {fds307586}
}

@article{fds313596,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
             M},
   Title = {Measurement of charged-particle spectra in Pb+Pb collisions
             at √sNN = 2.76 TeV with the ATLAS detector at the
             LHC},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {9},
   Pages = {1-51},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2015)050},
   Abstract = {Charged-particle spectra obtained in Pb+Pb interactions at
             (Formula presented.) and pp interactions at (Formula
             presented.) with the ATLAS detector at the LHC are
             presented, using data with integrated luminosities of 0.15
             nb−1 and 4.2 pb−1, respectively, in a wide transverse
             momentum (0.5 < pT< 150 GeV) and pseudorapidity (|η| < 2)
             range. For Pb+Pb collisions, the spectra are presented as a
             function of collision centrality, which is determined by the
             response of the forward calorimeters located on both sides
             of the interaction point. The nuclear modification factors
             RAA and RCP are presented in detail as a function of
             centrality, pT and η. They show a distinct pT-dependence
             with a pronounced minimum at about 7 GeV. Above 60 GeV, RAA
             is consistent with a plateau at a centrality-dependent
             value, within the uncertainties. The value is 0.55 ±
             0.01(stat.) ± 0.04(syst.) in the most central collisions.
             The RAA distribution is consistent with flat |η| dependence
             over the whole transverse momentum range in all centrality
             classes.},
   Doi = {10.1007/JHEP09(2015)050},
   Key = {fds313596}
}

@article{fds347481,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Coutinho,
             YA and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque,
             JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
             J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez,
             O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas,
             AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Gupta, DB and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce,
             M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos,
             N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertram, IA and Bertsche, C and Besjes, GJ and Bylund,
             OB and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
             AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov,
             A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow,
             TM and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
             D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana,
             S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo,
             FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati,
             L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Gimenez, VC and Castro,
             NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Barajas, CAC and Che, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen,
             H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
             YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
             YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară,
             IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Clark,
             A and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Colasurdo, L and Cole, B and Colijn, AP and Collot, J and Muiño, PC and Coniavitis, E and Connell,
             SH},
   Title = {Measurement of colour flow using jet-pull observables in t t
             ¯ events with the ATLAS experiment at s = 13
             TeV.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {10},
   Pages = {847},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-6290-2},
   Abstract = {Previous studies have shown that weighted angular moments
             derived from jet constituents encode the colour connections
             between partons that seed the jets. This paper presents
             measurements of two such distributions, the jet-pull angle
             and jet-pull magnitude, both of which are derived from the
             jet-pull angular moment. The measurement is performed in t t
             ¯ events with one leptonically decaying <i>W</i> boson and
             one hadronically decaying <i>W</i> boson, using 36.1 fb - 1
             of <i>pp</i> collision data recorded by the ATLAS detector
             at s = 13 TeV delivered by the Large Hadron Collider. The
             observables are measured for two dijet systems,
             corresponding to the colour-connected daughters of the
             <i>W</i> boson and the two <i>b</i>-jets from the top-quark
             decays, which are not expected to be colour connected. To
             allow the comparison of the measured distributions to colour
             model predictions, the measured distributions are unfolded
             to particle level, after correcting for experimental effects
             introduced by the detector. While good agreement can be
             found for some combinations of predictions and observables,
             none of the predictions describes the data well across all
             observables.},
   Doi = {10.1140/epjc/s10052-018-6290-2},
   Key = {fds347481}
}

@article{fds316569,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of colour flow with the jet pull angle in tt-
             events using the ATLAS detector at √s=8
             TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {750},
   Pages = {475-493},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {November},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.09.051},
   Abstract = {The distribution and orientation of energy inside jets is
             predicted to be an experimental handle on colour connections
             between the hard-scatter quarks and gluons initiating the
             jets. This Letter presents a measurement of the distribution
             of one such variable, the jet pull angle. The pull angle is
             measured for jets produced in tt- events with one W boson
             decaying leptonically and the other decaying to jets using
             20.3 fb-1 of data recorded with the ATLAS detector at a
             centre-of-mass energy of s=8 TeV at the LHC. The jet pull
             angle distribution is corrected for detector resolution and
             acceptance effects and is compared to various
             models.},
   Doi = {10.1016/j.physletb.2015.09.051},
   Key = {fds316569}
}

@article{fds307813,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'errico, M},
   Title = {Measurement of CP-violating asymmetries in D0→π
             +π - and D0→K +K
             - decays at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012009},
   Abstract = {We report on a measurement of CP-violating asymmetries (A
             CP) in the Cabibbo-suppressed D0→π +π - and D0→K +K -
             decays reconstructed in a data sample corresponding to 5.9fb
             -1 of integrated luminosity collected by the upgraded
             Collider Detector at Fermilab. We use the strong decay D
             *+→D0π + to identify the flavor of the charmed meson at
             production and exploit CP-conserving strong cc̄ pair
             production in pp̄ collisions. High-statistics samples of
             Cabibbo-favored D0→K -π + decays with and without a D *±
             tag are used to correct for instrumental effects and
             significantly reduce systematic uncertainties. We measure A
             CP(D0→π +π -)=(+0.22±0.24(stat) ±0.11(syst))% and A
             CP(D0→K +K -)=(-0.24±0.22(stat)±0.09(syst))%, in
             agreement with CP conservation. These are the most precise
             determinations from a single experiment to date. Under the
             assumption of negligible direct CP violation in D0→π +π
             - and D0→K +K - decays, the results provide an upper limit
             to the CP-violating asymmetry in D0 mixing,
             |ACPind(D0)|<0.13% at the 90% confidence level. © 2012
             American Physical Society.},
   Doi = {10.1103/PhysRevD.85.012009},
   Key = {fds307813}
}

@article{fds307823,
   Author = {Aaltonen, T and Ãlvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'Errico, M},
   Title = {Measurement of CP-violation asymmetries in D0→KS0π
             +π -},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.032007},
   Abstract = {We report a measurement of time-integrated CP-violation
             asymmetries in the resonant substructure of the three-body
             decay D0→KS0π +π - using CDF II data corresponding to
             6.0fb -1 of integrated luminosity from Tevatron pp̄
             collisions at √s=1.96TeV. The charm mesons used in this
             analysis come from D *+(2010) →D0π + and D *-(2010)→D
             ̄0π -, where the production flavor of the charm meson is
             determined by the charge of the accompanying pion. We apply
             a Dalitz-amplitude analysis for the description of the
             dynamic decay structure and use two complementary
             approaches, namely, a full Dalitz-plot fit employing the
             isobar model for the contributing resonances and a
             model-independent bin-by-bin comparison of the D0 and D ̄0
             Dalitz plots. We find no CP-violation effects and measure an
             asymmetry of A CP=(-0.05±0. 57(stat)±0.54(syst))% for the
             overall integrated CP-violation asymmetry, consistent with
             the standard model prediction. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.86.032007},
   Key = {fds307823}
}

@article{fds307998,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and González, BAL and Amerio,
             S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D},
   Title = {Measurement of cross sections for b jet production in events
             with a Z boson in pp̄ collisions at s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.052008},
   Abstract = {A measurement of the b jet production cross section is
             presented for events containing a Z boson produced in pp̄
             collisions at s=1.96TeV, using data corresponding to an
             integrated luminosity of 2fb-1 collected by the CDF II
             detector at the Tevatron. Z bosons are selected in the
             electron and muon decay modes. Jets are considered with
             transverse energy ET>20GeV and pseudorapidity |η|<1.5 and
             are identified as b jets using a secondary vertex algorithm.
             The ratio of the integrated Z+b jet cross section to the
             inclusive Z production cross section is measured to be
             3.32±0.53(stat)±0.42(syst) ×10-3. This ratio is also
             measured differentially in jet ET, jet η, Z-boson
             transverse momentum, number of jets, and number of b jets.
             The predictions from leading-order Monte Carlo generators
             and next-to-leading-order QCD calculations are found to be
             consistent with the measurements within experimental and
             theoretical uncertainties. © 2009 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.79.052008},
   Key = {fds307998}
}

@article{fds373544,
   Author = {Jackson, P and Kong, AXY and Oliver, JL and Ruggeri, TA and Sharma, AS and White, MJ and Jain, V and Swift, SP and Gingrich, DM and Pinfold, JL and Wang, H and Cakir, O and Duran Yildiz and H and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Belfkir, M and Berger, N and Costanza, F and Cueto, A and Dartsi, O and Delmastro, M and Di Ciaccio,
             L and Franco, L and Goy, C and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Lafaye, R and Levêque, J and Lorenzo
             Martinez, N and Portales, L and Sauvan, E and Wingerter-Seez, I and Abulaiti, Y and Benjamin, DP and Bhopatkar, VS and Chekanov, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe,
             J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Zhang, J and Berlendis, S and Cheu, E and Delitzsch, CM and Johns, KA and Lampl, W and LeBlanc, M and Lindley, RE and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave,
             B and De, K and Eifert, T and Farbin, A and Hadavand, HK and Little, JD and Ozturk, N and Usai, G and White, A and Angelidakis, S and Bellos, P and Fassouliotis, D and Gkialas, I and Kourkoumelis, C and Papageorgiou,
             K and Alexopoulos, T and Bakalis, C and Benekos, N and Gazis, EN and Gkountoumis, P and Kitsaki, C and Koulouris, A and Maltezos, S and Paraskevopoulos, C and Zacharis, G and Andeen, T and Burton, CD and Choi, K and Nikiforou, N and Onyisi, PUE and Potti, H and Roy, A and Unal,
             M and Webb, AF and Beddall, AJ and Celebi, E and Cetin,
             SA},
   Title = {Measurement of cross sections for production of a Z boson in
             association with a flavor-inclusive or doubly b-tagged
             large-radius jet in proton-proton collisions at √s = 13
             TeV with the ATLAS experiment},
   Journal = {Physical Review D},
   Volume = {108},
   Number = {1},
   Year = {2023},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.108.012022},
   Abstract = {We present measurements of cross sections for production of
             a leptonically decaying Z boson in association with a
             large-radius jet in 13 TeV proton-proton collisions at the
             LHC, using 36 fb - 1 of data from the ATLAS detector.
             Integrated and differential cross sections are measured at
             particle level in both a flavor inclusive and a doubly b
             -tagged fiducial phase space. The large-radius jet mass and
             transverse momentum, its kinematic relationship to the Z
             boson, and the angular separation of b -tagged small-radius
             track jets within the large-radius jet are measured. This
             measurement constitutes an important test of perturbative
             quantum chromodynamics in kinematic and flavor
             configurations relevant to several Higgs boson and
             beyond-Standard-Model physics analyses. The results
             highlight issues with modeling of additional hadronic
             activity in the flavor-inclusive selection, and a
             distinction between flavor-number schemes in the b -tagged
             phase space.},
   Doi = {10.1103/PhysRevD.108.012022},
   Key = {fds373544}
}

@article{fds307746,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Kesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni,
             G and Arutinov, D},
   Title = {Measurement of D  meson production in jets
             from pp collisions at √s=7TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.052005},
   Abstract = {This paper reports a measurement of D *± meson production
             in jets from proton-proton collisions at a center-of-mass
             energy of √s=7TeV at the CERN Large Hadron Collider. The
             measurement is based on a data sample recorded with the
             ATLAS detector with an integrated luminosity of 0.30pb -1
             for jets with transverse momentum between 25 and 70 GeV in
             the pseudorapidity range |η|<2.5. D *± mesons found in
             jets are fully reconstructed in the decay chain: D *+→D0π
             +, D0→K -π +, and its charge conjugate. The production
             rate is found to be N(D *±)/N(jet)=0.025±0.
             001(stat.)±0.004(syst.) for D *± mesons that carry a
             fraction z of the jet momentum in the range 0.3<z<1. Monte
             Carlo predictions fail to describe the data at small values
             of z, and this is most marked at low jet transverse
             momentum. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.85.052005},
   Key = {fds307746}
}

@article{fds315922,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of D⁎±, D± and
             Ds± meson production cross sections
             in pp collisions at √s=7 TeV with the ATLAS
             detector},
   Journal = {Nuclear Physics B},
   Volume = {907},
   Pages = {717-763},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {June},
   ISSN = {0550-3213},
   url = {http://dx.doi.org/10.1016/j.nuclphysb.2016.04.032},
   Abstract = {The production of D⁎±, D± and Ds± charmed mesons has
             been measured with the ATLAS detector in pp collisions at
             s=7 TeV at the LHC, using data corresponding to an
             integrated luminosity of 280 nb−1. The charmed mesons have
             been reconstructed in the range of transverse momentum
             3.5<pT(D)<100 GeV and pseudorapidity |η(D)|<2.1. The
             differential cross sections as a function of transverse
             momentum and pseudorapidity were measured for D⁎± and D±
             production. The next-to-leading-order QCD predictions are
             consistent with the data in the visible kinematic region
             within the large theoretical uncertainties. Using the
             visible D cross sections and an extrapolation to the full
             kinematic phase space, the strangeness-suppression factor in
             charm fragmentation, the fraction of charged non-strange D
             mesons produced in a vector state, and the total cross
             section of charm production at s=7 TeV were
             derived.},
   Doi = {10.1016/j.nuclphysb.2016.04.032},
   Key = {fds315922}
}

@article{fds347492,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic,
             M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz,
             T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black,
             KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou,
             Y},
   Title = {Measurement of detector-corrected observables sensitive to
             the anomalous production of events with jets and large
             missing transverse momentum in p p collisions at s = 13
              TeV using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {11},
   Pages = {765},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5315-6},
   Abstract = {Observables sensitive to the anomalous production of events
             containing hadronic jets and missing momentum in the plane
             transverse to the proton beams at the Large Hadron Collider
             are presented. The observables are defined as a ratio of
             cross sections, for events containing jets and large missing
             transverse momentum to events containing jets and a pair of
             charged leptons from the decay of a Z / γ ∗ boson. This
             definition minimises experimental and theoretical systematic
             uncertainties in the measurements. This ratio is measured
             differentially with respect to a number of kinematic
             properties of the hadronic system in two phase-space
             regions; one inclusive single-jet region and one region
             sensitive to vector-boson-fusion topologies. The data are
             found to be in agreement with the Standard Model predictions
             and used to constrain a variety of theoretical models for
             dark-matter production, including simplified models,
             effective field theory models, and invisible decays of the
             Higgs boson. The measurements use 3.2 fb - 1 of
             proton-proton collision data recorded by the ATLAS
             experiment at a centre-of-mass energy of 13  TeV and are
             fully corrected for detector effects, meaning that the data
             can be used to constrain new-physics models beyond those
             shown in this paper.},
   Doi = {10.1140/epjc/s10052-017-5315-6},
   Key = {fds347492}
}

@article{fds356685,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
             P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of differential cross sections and W
             + /W  cross-section ratios for W
             boson production in association with jets at √s=8 TeV with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {5},
   Year = {2018},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2018)077},
   Abstract = {This paper presents a measurement of the W boson production
             cross section and the W+/W− cross-section ratio, both in
             association with jets, in proton-proton collisions at s=8
             TeV with the ATLAS experiment at the Large Hadron Collider.
             The measurement is performed in final states containing one
             electron and missing transverse momentum using data
             corresponding to an integrated luminosity of 20.2 fb−1.
             Differential cross sections for events with at least one or
             two jets are presented for a range of observables, including
             jet transverse momenta and rapidities, the scalar sum of
             transverse momenta of the visible particles and the missing
             transverse momentum in the event, and the transverse
             momentum of the W boson. For a subset of the observables,
             the differential cross sections of positively and negatively
             charged W bosons are measured separately. In the
             cross-section ratio of W+/W− the dominant systematic
             uncertainties cancel out, improving the measurement
             precision by up to a factor of nine. The observables and
             ratios selected for this paper provide valuable input for
             the up quark, down quark, and gluon parton distribution
             functions of the proton.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP05(2018)077},
   Key = {fds356685}
}

@article{fds356542,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
             V},
   Title = {Measurement of differential cross sections for single
             diffractive dissociation in √s = 8 TeV pp collisions using
             the ATLAS ALFA spectrometer},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {2},
   Year = {2020},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP02(2020)042},
   Abstract = {A dedicated sample of Large Hadron Collider proton-proton
             collision data at centre-of-mass energy s = 8 TeV is used to
             study inclusive single diffractive dissociation, pp → X p.
             The intact final-state proton is reconstructed in the ATLAS
             ALFA forward spectrometer, while charged particles from the
             dissociated system X are measured in the central detector
             components. The fiducial range of the measurement is −4.0
             < log10ξ < −1.6 and 0.016 < |t| < 0.43 GeV2, where ξ is
             the proton fractional energy loss and t is the squared
             four-momentum transfer. The total cross section integrated
             across the fiducial range is 1.59 ± 0.13 mb. Cross sections
             are also measured differentially as functions of ξ, t, and
             ∆η, a variable that characterises the rapidity gap
             separating the proton and the system X. The data are
             consistent with an exponential t dependence, dσ/dt ∝ eBt
             with slope parameter B = 7.65 ± 0.34 GeV−2. Interpreted
             in the framework of triple Regge phenomenology, the ξ
             dependence leads to a pomeron intercept of α(0) = 1.07 ±
             0.09. [Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP02(2020)042},
   Key = {fds356542}
}

@article{fds356700,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
             P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of differential cross sections of
             isolated-photon plus heavy-flavour jet production in pp
             collisions at s=8 TeV using the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {776},
   Pages = {295-317},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2017.11.054},
   Abstract = {This Letter presents the measurement of differential cross
             sections of isolated prompt photons produced in association
             with a b-jet or a c-jet. These final states provide
             sensitivity to the heavy-flavour content of the proton and
             aspects related to the modelling of heavy-flavour quarks in
             perturbative QCD. The measurement uses proton–proton
             collision data at a centre-of-mass energy of 8 TeV recorded
             by the ATLAS detector at the LHC in 2012 corresponding to an
             integrated luminosity of up to 20.2 fb−1. The differential
             cross sections are measured for each jet flavour with
             respect to the transverse energy of the leading photon in
             two photon pseudorapidity regions: |ηγ|<1.37 and
             1.56<|ηγ|<2.37. The measurement covers photon transverse
             energies 25<ETγ<400 GeV and 25<ETγ<350 GeV respectively
             for the two |ηγ| regions. For each jet flavour, the ratio
             of the cross sections in the two |ηγ| regions is also
             measured. The measurement is corrected for detector effects
             and compared to leading-order and next-to-leading-order
             perturbative QCD calculations, based on various treatments
             and assumptions about the heavy-flavour content of the
             proton. Overall, the predictions agree well with the
             measurement, but some deviations are observed at high photon
             transverse energies. The total uncertainty in the
             measurement ranges between 13% and 66%, while the central
             γ+b measurement exhibits the smallest uncertainty, ranging
             from 13% to 27%, which is comparable to the precision of the
             theoretical predictions.},
   Doi = {10.1016/j.physletb.2017.11.054},
   Key = {fds356700}
}

@article{fds347472,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
             P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
             H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
             C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
             AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
             O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
             D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Li, C-Q and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho
             Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and CapeansGarrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo,
             F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati,
             L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and CastilloGimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
             YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
             YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran,
             J},
   Title = {Measurement of differential cross-sections of a single top
             quark produced in association with a W boson at s =
             13 TeV with ATLAS.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {3},
   Pages = {186},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-5649-8},
   Abstract = {The differential cross-section for the production of a
             <i>W</i> boson in association with a top quark is measured
             for several particle-level observables. The measurements are
             performed using 36.1 fb - 1 of <i>pp</i> collision data
             collected with the ATLAS detector at the LHC in 2015 and
             2016. Differential cross-sections are measured in a fiducial
             phase space defined by the presence of two charged leptons
             and exactly one jet matched to a <i>b</i>-hadron, and are
             normalised with the fiducial cross-section. Results are
             found to be in good agreement with predictions from several
             Monte Carlo event generators.},
   Doi = {10.1140/epjc/s10052-018-5649-8},
   Key = {fds347472}
}

@article{fds313616,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Measurement of differential J/ψ production cross sections
             and forward-backward ratios in p + Pb collisions with the
             ATLAS detector},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {92},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {October},
   ISSN = {0556-2813},
   url = {http://dx.doi.org/10.1103/PhysRevC.92.034904},
   Abstract = {Measurements of differential cross sections for J/ψ
             production in p + Pb collisions at (√SNN at the CERN Large
             Hadron Collider with the ATLAS detector are presented. The
             data set used corresponds to an integrated luminosity of
             28.1 nb−1. The J/ψ mesons are reconstructed in the dimuon
             decay channel over the transverse momentum range 8 < pT < 30
             GeV and over the center-of-mass rapidity range −2.87 <
             y∗ < 1.94. Prompt J/ψ are separated from J/ψ resulting
             from b-hadron decays through an analysis of the distance
             between the J/ψ decay vertex and the event primary vertex.
             The differential cross section for production of nonprompt
             J/ψ is compared to a FONLL calculation that does not
             include nuclear effects. Forward-backward production ratios
             are presented and compared to theoretical predictions. These
             results complement previously published results by covering
             a region of higher transverse momentum and more central
             rapidity. They thus constrain the kinematic dependence of
             nuclear modifications of charmonium and b-quark production
             in p + Pb collisions.},
   Doi = {10.1103/PhysRevC.92.034904},
   Key = {fds313616}
}

@article{fds310335,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JJA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Measurement of differential production cross sections for Z
             /γ∗ bosons in association with jets in p p ¯ collisions
             at s =1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.012002},
   Abstract = {Differential cross sections for the production of Z bosons
             or off-shell photons γ∗ in association with jets are
             measured in proton-antiproton collisions at center-of-mass
             energy s=1.96TeV using the full data set collected with the
             Collider Detector at Fermilab in Tevatron run II and
             corresponding to 9.6fb-1 of integrated luminosity. Results
             include first measurements at CDF of differential cross
             sections in events with a Z/γ∗ boson and three or more
             jets, the inclusive cross section for production of Z/γ∗
             and four or more jets, and cross sections as functions of
             various angular observables in lower jet-multiplicity final
             states. Measured cross sections are compared to several
             theoretical predictions.},
   Doi = {10.1103/PhysRevD.91.012002},
   Key = {fds310335}
}

@article{fds310356,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of differential production cross-sections for a
             Z boson in association with b-jets in 7 TeV proton-proton
             collisions with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {10},
   Pages = {1-49},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2014)141},
   Abstract = {Abstract: Measurements of differential production
             cross-sections of a Z boson in association with b-jets in pp
             collisions at √ = 7 TeV are reported. The data analysed
             correspond to an integrated luminosity of 4.6 fb−1
             recorded with the ATLAS detector at the Large Hadron
             Collider. Particle-level cross-sections are determined for
             events with a Z boson decaying into an electron or muon
             pair, and containing b-jets. For events with at least one
             b-jet, the cross-section is presented as a function of the Z
             boson transverse momentum and rapidity, together with the
             inclusive b-jet cross-section as a function of b-jet
             transverse momentum, rapidity and angular separations
             between the b-jet and the Z boson. For events with at least
             two b-jets, the cross-section is determined as a function of
             the invariant mass and angular separation of the two highest
             transverse momentum b-jets, and as a function of the Z boson
             transverse momentum and rapidity. Results are compared to
             leading-order and next-to-leading-order perturbative QCD
             calculations.},
   Doi = {10.1007/JHEP10(2014)141},
   Key = {fds310356}
}

@booklet{Abbott98o,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
             V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
             C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
             P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
             MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
             G and Fisk, HE and Fisyak, Y and Flattum, E},
   Title = {Measurement of dijet angular distributions and search for
             quark compositeness},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {4},
   Pages = {666-671},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.666},
   Abstract = {We have measured the dijet angular distribution in s = 1.8
             TeV pp collisions using the D0 detector. Order αs3 QCD
             predictions are in good agreement with the data. At 95%
             confidence limit the data exclude models of quark
             compositeness in which the contact interaction scale is
             below 2 TeV. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.80.666},
   Key = {Abbott98o}
}

@article{fds308132,
   Author = {Abazov, VM and Abbott, B and Abolins, M and Acharya, BS and Adams, DL and Adams, M and Adams, T and Agelou, M and Agram, J-L and Ahmed, SN and Ahn,
             SH and Alexeev, GD and Alkhazov, G and Alton, A and Alverson, G and Alves,
             GA and Anastasoaie, M and Anderson, S and Andrieu, B and Arnoud, Y and Askew, A and Asman, B and Atramentov, O and Autermann, C and Avila, C and Babukhadia, L and Bacon, TC and Badaud, F and Baden, A and Baffioni, S and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Bargassa, P and Baringer, P and Barnes, C and Barreto, J and Bartlett, JF and Bassler,
             U and Bauer, D and Bean, A and Beauceron, S and Beaudette, F and Begel, M and Bellavance, A and Beri, SB and Bernardi, G and Bernhard, R and Bertram,
             I and Besançon, M and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Binder, M and Bischoff, A and Black, KM and Blackler, I and Blazey, G and Blekman, F and Blessing, S and Bloch, D and Blumenschein, U and Boehnlein, A and Boeriu, O and Bolton, TA and Bonamy, P and Borcherding, F and Borissov,
             G and Bos, K and Bose, T and Boswell, C and Brandt, A and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchanan, NJ and Buchholz,
             D and Buehler, M and Buescher, V and Burdin, S and Burnett, TH and Busato,
             E and Butler, JM and Bystricky, J and Canelli, F and Carvalho, W and Casey,
             BCK and Casey, D and Cason, NM and Castilla-Valdez, H and Chakrabarti,
             S and Chakraborty, D and Chan, KM and Chandra, A and Chapin, D and Charles,
             F and Cheu, E and Chevalier, L and Cho, DK and Choi, S and Chopra, S and Christiansen, T and Christofek, L and Claes, D and Clark, AR and Clément, B and Clément, C and Coadou, Y and Colling, DJ and Coney, L and Connolly, B and Cooke, M and Cooper, WE and Coppage, D and Corcoran, M and Coss, J and Cothenet, A and Cousinou, M-C and Crépé-Renaudin, S and Cristetiu, M and Cummings, MAC and Cutts, D and da Motta, H and Davies,
             B and Davies, G and Davis, GA and De, K and de Jong, P and de Jong, SJ and De
             La Cruz-Burelo and E and Martins, CDO and Dean, S and Del Signore and K and Déliot, F and Delsart, PA and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doidge, M and Dong, H and Doulas, S and Duflot, L and Dugad, SR and Duperrin, A and Dyer, J and Dyshkant, A and Eads, M and Edmunds, D and Edwards, T and Ellison, J and Elmsheuser, J and Eltzroth, JT and Elvira,
             VD and Eno, S and Ermolov, P and Eroshin, OV and Estrada, J and Evans, D and Evans, H and Evdokimov, A and Evdokimov, VN and Fast, J and Fatakia, SN and Fein, D and Feligioni, L and Ferbel, T and Fiedler, F and Filthaut, F and Fisher, W and Fisk, HE and Fleuret, F and Fortner, M and Fox, H and Freeman, W and Fu, S and Fuess, S and Galea, CF and Gallas, E and Galyaev,
             E and Gao, M and Garcia, C and Garcia-Bellido, A and Gardner, J and Gavrilov, V and Gay, P and Gelé, D and Gelhaus, R and Genser, K and Gerber, CE and Gershtein, Y and Geurkov, G and Ginther, G and Goldmann,
             K and Golling, T and Gómez, B and Gounder, K and Goussiou, A and Graham,
             G and Grannis, PD and Greder, S and Green, JA and Greenlee, H and Greenwood, ZD and Gregores, EM and Grinstein, S and Gris, P and Grivaz,
             J-F and Groer, L and Grünendahl, S and Grünewald, MW and Gu, W and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Haas, A and Hadley,
             NJ and Haggerty, H and Hagopian, S and Hall, I and Hall, RE and Han, C and Han, L and Hanagaki, K and Hanlet, P and Harder, K and Harrington, R and Hauptman, JM and Hauser, R and Hays, C and Hays, J and Hebbeker, T and Hebert, C and Hedin, D and Heinmiller, JM and Heinson, AP and Heintz, U and Hensel, C and Hesketh, G and Hildreth, MD and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hohlfeld, M and Hong, SJ and Hooper, R and Hou, S and Houben, P and Hu, Y and Huang, J and Huang, Y and Iashvili, I and Illingworth, R and Ito, AS and Jabeen, S and Jaffré, M and Jain, S and Jain, V and Jakobs, K and Jenkins, A and Jesik, R and Jiang, Y and Johns,
             K and Johnson, M and Johnson, P and Jonckheere, A and Jonsson, P and Jöstlein, H and Juste, A and Kado, MM and Käfer, D and Kahl, W and Kahn,
             S and Kajfasz, E and Kalinin, AM and Kalk, J and Karmanov, D and Kasper, J and Kau, D and Ke, Z and Kehoe, R and Kermiche, S and Kesisoglou, S and Khanov,
             A and Kharchilava, A and Kharzheev, YM and Kim, KH and Klima, B and Klute,
             M and Kohli, JM and Kopal, M and Korablev, VM and Kotcher, J and Kothari,
             B and Kotwal, AV and Koubarovsky, A and Kouznetsov, O and Kozelov, AV and Kozminski, J and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kurca, T and Kuznetsov, VE and Lager, S and Lahrichi, N and Landsberg,
             G and Lazoflores, J and Le Bihan and A-C and Lebrun, P and Lee, SW and Lee,
             WM and Leflat, A and Leggett, C and Lehner, F and Leonidopoulos, C and Lewis, P and Li, J and Li, QZ and Li, X and Lima, JGR and Lincoln, D and Linn,
             SL and Linnemann, J and Lipaev, VV and Lipton, R and Lobo, L and Lobodenko,
             A and Lokajicek, M and Lounis, A and Lu, J and Lubatti, HJ and Lucotte, A and Lueking, L and Luo, C and Lynker, M and Lyon, AL and Maciel, AKA and Madaras, RJ and Mättig, P and Magerkurth, A and Magnan, A-M and Maity,
             M and Makovec, N and Mal, PK and Malik, S and Malyshev, VL and Manankov, V and Mao, HS and Maravin, Y and Marshall, T and Martens, M and Martin, MI and Mattingly, SEK and Mayorov, AA and McCarthy, R and McCroskey, R and McMahon, T and Meder, D and Melanson, HL and Melnitchouk, A and Meng, X and Merkin, M and Merritt, KW and Meyer, A and Miao, C and Miettinen, H and Mihalcea, D and Mitrevski, J and Mokhov, N and Molina, J and Mondal, NK and Montgomery, HE and Moore, RW and Mostafa, M and Muanza, GS and Mulders,
             M and Mutaf, YD and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Naumann, NA and Neal, HA and Negret, JP and Nelson, S and Neustroev, P and Noeding, C and Nomerotski, A and Novaes, SF and Nunnemann, T and Nurse,
             E and O'Dell, V and O'Neil, DC and Oguri, V and Oliveira, N and Olivier, B and Oshima, N and Otero y Garzón and GJ and Padley, P and Papageorgiou, K and Parashar, N and Park, J and Park, SK and Parsons, J and Partridge, R and Parua, N and Patwa, A and Perea, PM and Perez, E and Peters, O and Pétroff, P and Petteni, M and Phaf, L and Piegaia, R and Podesta-Lerma,
             PLM and Podstavkov, VM and Pogorelov, Y and Pope, BG and Popkov, E and Prado da Silva and WL and Prosper, HB and Protopopescu, S and Przybycien, MB and Qian, J and Quadt, A and Quinn, B and Rani, KJ and Rapidis, PA and Ratoff, PN and Reay, NW and Renardy, J-F and Reucroft,
             S and Rha, J and Ridel, M and Rijssenbeek, M and Ripp-Baudot, I and Rizatdinova, F and Royon, C and Rubinov, P and Ruchti, R and Sabirov,
             BM and Sajot, G and Sánchez-Hernández, A and Sanders, MP and Santoro,
             A and Savage, G and Sawyer, L and Scanlon, T and Schamberger, RD and Schellman, H and Schieferdecker, P and Schmitt, C and Schukin, AA and Schwartzman, A and Schwienhorst, R and Sengupta, S and Severini, H and Shabalina, E and Shary, V and Shephard, WD and Shpakov, D and Sidwell,
             RA and Simak, V and Sirotenko, V and Skow, D and Skubic, P and Slattery, P and Smith, RP and Smolek, K and Snow, GR and Snow, J and Snyder, S and Söldner-Rembold, S and Song, X and Song, Y and Sonnenschein, L and Sopczak, A and Sorín, V and Sosebee, M and Soustruznik, K and Souza, M and Spurlock, B and Stanton, NR and Stark, J and Steele,
             J},
   Title = {Measurement of dijet azimuthal decorrelations at central
             rapidities in pp collisions at sqrt s =1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {94},
   Number = {22},
   Pages = {221801},
   Year = {2005},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.94.221801},
   Abstract = {Correlations in the azimuthal angle between the two largest
             transverse momentum jets have been measured using the D0
             detector in p (-)p collisions at a center-of-mass energy
             sqrt[s]=1.96 TeV. The analysis is based on an inclusive
             dijet event sample in the central rapidity region
             corresponding to an integrated luminosity of 150 pb(-1).
             Azimuthal correlations are stronger at larger transverse
             momenta. These are well described in perturbative QCD at
             next-to-leading order in the strong coupling constant,
             except at large azimuthal differences where contributions
             with low transverse momentum are significant.},
   Doi = {10.1103/physrevlett.94.221801},
   Key = {fds308132}
}

@article{fds356643,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson,
             TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold,
             H},
   Title = {Measurement of dijet azimuthal decorrelations in pp
             collisions at s =8 TeV with the ATLAS detector and
             determination of the strong coupling},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {9},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.092004},
   Abstract = {A measurement of the rapidity and transverse momentum
             dependence of dijet azimuthal decorrelations is presented,
             using the quantity RΔφ. The quantity RΔφ specifies the
             fraction of the inclusive dijet events in which the
             azimuthal opening angle of the two jets with the highest
             transverse momenta is less than a given value of the
             parameter Δφmax. The quantity RΔφ is measured in
             proton-proton collisions at s=8 TeV as a function of the
             dijet rapidity interval, the event total scalar transverse
             momentum, and Δφmax. The measurement uses an event sample
             corresponding to an integrated luminosity of 20.2 fb-1
             collected with the ATLAS detector at the CERN Large Hadron
             Collider. Predictions of a perturbative QCD calculation at
             next-to-leading order in the strong coupling with
             corrections for nonperturbative effects are compared to the
             data. The theoretical predictions describe the data in the
             whole kinematic region. The data are used to determine the
             strong coupling αS and to study its running for momentum
             transfers from 260 GeV to above 1.6 TeV. Analysis that
             combines data at all momentum transfers results in
             αS(mZ)=0.1127-0.0027+0.0063.},
   Doi = {10.1103/PhysRevD.98.092004},
   Key = {fds356643}
}

@article{fds310380,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin,
             JF},
   Title = {Measurement of dijet cross-sections in pp collisions at 7
             TeV centre-of-mass energy using the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP05(2014)059},
   Abstract = {Double-differential dijet cross-sections measured in pp
             collisions at the LHC with a 7TeV centre-of-mass energy are
             presented as functions of dijet mass and half the rapidity
             separation of the two highest-pT jets. These measurements
             are obtained using data corresponding to an integrated
             luminosity of 4.5 fb−1, recorded by the ATLAS detector in
             2011. The data are corrected for detector effects so that
             cross-sections are presented at the particle level.
             Cross-sections are measured up to 5TeV dijet mass using jets
             reconstructed with the anti-kt algorithm for values of the
             jet radius parameter of 0.4 and 0.6. The cross-sections are
             compared with next-to-leading-order perturbative QCD
             calculations by NLOJet++ corrected to account for
             non-perturbative effects. Comparisons with POWHEG
             predictions, using a next-to-leading-order matrix element
             calculation interfaced to a partonshower Monte Carlo
             simulation, are also shown. Electroweak effects are
             accounted for in both cases. The quantitative comparison of
             data and theoretical predictions obtained using various
             parameterizations of the parton distribution functions is
             performed using a frequentist method. In general, good
             agreement with data is observed for the NLOJet++ theoretical
             predictions when using the CT10, NNPDF2.1 and MSTW 2008 PDF
             sets. Disagreement is observed when using the ABM11 and
             HERAPDF1.5 PDF sets for some ranges of dijet mass and half
             the rapidity separation. An example setting a lower limit on
             the compositeness scale for a model of contact interactions
             is presented, showing that the unfolded results can be used
             to constrain contributions to dijet production beyond that
             predicted by the Standard Model.},
   Doi = {10.1007/JHEP05(2014)059},
   Key = {fds310380}
}

@article{fds321141,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of dijet production with a veto on additional
             central jet activity in pp collisions at √s = 7TeV using
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2011},
   Number = {9},
   Pages = {1-36},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP09(2011)053},
   Abstract = {A measurement of jet activity in the rapidity interval
             bounded by a dijet system is presented. Events are vetoed if
             a jet with transverse momentum greater than 20GeV is found
             between the two boundary jets. The fraction of dijet events
             that survive the jet veto is presented for boundary jets
             that are separated by up to six units of rapidity and with
             mean transverse momentum 50 < pT < 500GeV. The mean
             multiplicity of jets above the veto scale in the rapidity
             interval bounded by the dijet system is also presented as an
             alternative method for quantifying perturbative QCD
             emission. The data are compared to a next-to-leading order
             plus parton shower prediction from the powheg-box, an
             all-order resummation using the hej calculation and the
             pythia, herwig++ and alpgen event generators. The
             measurement was performed using pp collisions at √s = 7TeV
             using data recorded by the ATLAS detector in
             2010.},
   Doi = {10.1007/JHEP09(2011)053},
   Key = {fds321141}
}

@article{fds356583,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
             L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
             JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA},
   Title = {Measurement of distributions sensitive to the underlying
             event in inclusive Z boson production in pp collisions at
             √s = 13 TeV with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {8},
   Year = {2019},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7162-0},
   Abstract = {This paper presents measurements of charged-particle
             distributions sensitive to the properties of the underlying
             event in events containing a Z boson decaying into a muon
             pair. The data were obtained using the ATLAS detector at the
             LHC in proton–proton collisions at a centre-of-mass energy
             of 13 Te with an integrated luminosity of 3.2fb-1.
             Distributions of the charged-particle multiplicity and of
             the charged-particle transverse momentum are measured in
             regions of the azimuth defined relative to the Z boson
             direction. The measured distributions are compared with the
             predictions of various Monte Carlo generators which
             implement different underyling event models. The Monte Carlo
             model predictions qualitatively describe the data well, but
             with some significant discrepancies.},
   Doi = {10.1140/epjc/s10052-019-7162-0},
   Key = {fds356583}
}

@article{fds310388,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Measurement of distributions sensitive to the underlying
             event in inclusive Z-boson production in [Formula: see text]
             collisions at [Formula: see text] TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {12},
   Pages = {3195},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3195-6},
   Abstract = {A measurement of charged-particle distributions sensitive to
             the properties of the underlying event is presented for an
             inclusive sample of events containing a [Formula: see
             text]-boson, decaying to an electron or muon pair. The
             measurement is based on data collected using the ATLAS
             detector at the LHC in proton-proton collisions at a
             centre-of-mass energy of [Formula: see text] TeV with an
             integrated luminosity of [Formula: see text] fb[Formula:
             see text]. Distributions of the charged particle
             multiplicity and of the charged particle transverse momentum
             are measured in regions of azimuthal angle defined with
             respect to the [Formula: see text]-boson direction. The
             measured distributions are compared to similar distributions
             measured in jet events, and to the predictions of various
             Monte Carlo generators implementing different underlying
             event models.},
   Doi = {10.1140/epjc/s10052-014-3195-6},
   Key = {fds310388}
}

@article{fds307923,
   Author = {Aaltonen, T and Adelman, J and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Appel, J and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
             S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway,
             J},
   Title = {Measurement of dσ/dy of Drell-Yan e+e-
             pairs in the Z mass region from pp̄ collisions at √s=1.96
             TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {692},
   Number = {4},
   Pages = {232-239},
   Publisher = {Elsevier BV},
   Year = {2010},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2010.06.043},
   Abstract = {We report on a CDF measurement of the total cross section
             and rapidity distribution, dσ/dy, for γ*Z→e+e- events in
             the Z boson mass region (66<Mee<116 GeV/c2) produced in pp-
             collisions at s=1.96 TeV with 2.1 fb-1 of integrated
             luminosity. The measured cross section of 257±16 pb and
             dσ/dy distribution are compared with Next-to-Leading-Order
             (NLO) and Next-to-Next-to-Leading-Order (NNLO) QCD theory
             predictions with CTEQ and MRST/MSTW parton distribution
             functions (PDFs). There is good agreement between the
             experimental total cross section and dσ/dy measurements
             with theoretical calculations with the most recent NNLO
             PDFs. © 2010 Elsevier B.V.},
   Doi = {10.1016/j.physletb.2010.06.043},
   Key = {fds307923}
}

@article{fds307676,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {Measurement of event shapes at large momentum transfer with
             the ATLAS detector in pp collisions at √s =7
             TeV},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2211-y},
   Abstract = {A measurement of event shape variables is presented for
             large momentum transfer proton-proton collisions using the
             ATLAS detector at the Large Hadron Collider. Six event shape
             variables calculated using hadronic jets are studied in
             inclusive multi-jet events in 35 pb<sup>-1</sup> of
             integrated luminosity at a center-of-mass energy of √s = 7
             TeV. These measurements are compared to predictions by three
             Monte Carlo event generators containing leading-logarithmic
             parton showers matched to leading order matrix elements for
             2→2 and 2→n (n = 2, …, 6) scattering. Measurements of
             the third-jet resolution parameter, aplanarity, thrust,
             sphericity, and transverse sphericity are generally well
             described. The mean value of each event shape variable is
             evaluated as a function of the average momentum of the two
             leading jets p<inf>T,1</inf> and p<inf>T,2</inf>, with a
             mean pT approaching 1 TeV.},
   Doi = {10.1140/epjc/s10052-012-2211-y},
   Key = {fds307676}
}

@article{fds307883,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of event shapes in $p\overline{p}$ collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {11},
   Pages = {112007},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.112007},
   Abstract = {A study of event-shape observables in proton-antiproton
             collisions at √s=1.96TeV is presented. The data for this
             analysis were recorded by the CDF II Detector at the
             Tevatron Collider. The variables studied are the transverse
             thrust and thrust minor, both defined in the plane
             perpendicular to the beam direction. The observables are
             measured using energies from unclustered calorimeter cells.
             In addition to studies of the differential distributions, we
             present the dependence of event-shape mean values on the
             leading-jet transverse energy. Data are compared with pythia
             Tune A and to resummed parton-level predictions that were
             matched to fixed-order results at next-to-leading-order
             (NLO) accuracy (NLO+NLL). Predictions from pythia Tune A
             agree fairly well with the data. However, the underlying
             event contributes significantly to these observables, making
             it difficult to make direct comparisons to the NLO+NLL
             predictions, which do not account for the underlying event.
             To overcome this difficulty, we introduce a new observable,
             a weighted difference of the mean values of the thrust and
             thrust minor, which is less sensitive to the underlying
             event, allowing for a comparison with NLO+NLL. Both pythia
             Tune A and the NLO+NLL calculations agree well within the
             20% theoretical uncertainty with the data for this
             observable, indicating that perturbative QCD successfully
             describes shapes of the hadronic final states. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.83.112007},
   Key = {fds307883}
}

@article{fds310369,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnal, V},
   Title = {Measurement of event-plane correlations in √sNN
             = 2.76 TeV lead-lead collisions with the ATLAS
             detector},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {90},
   Number = {2},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevC.90.024905},
   Abstract = {A measurement of event-plane correlations involving two or
             three event planes of different order is presented as a
             function of centrality for 7 μb-1 Pb+Pb collision data at
             sNN=2.76 TeV, recorded by the ATLAS experiment at the Large
             Hadron Collider. Fourteen correlators are measured using a
             standard event-plane method and a scalar-product method, and
             the latter method is found to give a systematically larger
             correlation signal. Several different trends in the
             centrality dependence of these correlators are observed.
             These trends are not reproduced by predictions based on the
             Glauber model, which includes only the correlations from the
             collision geometry in the initial state. Calculations that
             include the final-state collective dynamics are able to
             describe qualitatively, and in some cases also
             quantitatively, the centrality dependence of the measured
             correlators. These observations suggest that both the
             fluctuations in the initial geometry and the nonlinear
             mixing between different harmonics in the final state are
             important for creating these correlations in momentum
             space.},
   Doi = {10.1103/PhysRevC.90.024905},
   Key = {fds310369}
}

@article{fds321116,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
             Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
             De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
             TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ},
   Title = {Measurement of event-shape observables in [Formula: see
             text] events in pp collisions at [Formula: see
             text] [Formula: see text] with the ATLAS detector at the
             LHC.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {7},
   Pages = {375},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4176-8},
   Abstract = {Event-shape observables measured using charged particles in
             inclusive <i>Z</i>-boson events are presented, using the
             electron and muon decay modes of the <i>Z</i> bosons. The
             measurements are based on an integrated luminosity of
             [Formula: see text] of proton-proton collisions recorded by
             the ATLAS detector at the LHC at a centre-of-mass energy
             [Formula: see text] [Formula: see text]. Charged-particle
             distributions, excluding the lepton-antilepton pair from the
             <i>Z</i>-boson decay, are measured in different ranges of
             transverse momentum of the <i>Z</i> boson. Distributions
             include multiplicity, scalar sum of transverse momenta, beam
             thrust, transverse thrust, spherocity, and [Formula: see
             text]-parameter, which are in particular sensitive to
             properties of the underlying event at small values of the
             <i>Z</i>-boson transverse momentum. The measured observables
             are compared with predictions from Pythia 8, Sherpa, and
             Herwig 7. Typically, all three Monte Carlo generators
             provide predictions that are in better agreement with the
             data at high <i>Z</i>-boson transverse momenta than at low
             <i>Z</i>-boson transverse momenta, and for the observables
             that are less sensitive to the number of charged particles
             in the event.},
   Doi = {10.1140/epjc/s10052-016-4176-8},
   Key = {fds321116}
}

@article{fds371907,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
             A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
             W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
             MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
   Title = {Measurement of exclusive pion pair production in
             proton–proton collisions at √s=7TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {7},
   Year = {2023},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11700-x},
   Abstract = {The exclusive production of pion pairs in the process pp→
             ppπ+π- has been measured at s=7TeV with the ATLAS detector
             at the LHC, using 80μb-1 of low-luminosity data. The pion
             pairs were detected in the ATLAS central detector while
             outgoing protons were measured in the forward ATLAS ALFA
             detector system. This represents the first use of proton
             tagging to measure an exclusive hadronic final state at the
             LHC. A cross-section measurement is performed in two
             kinematic regions defined by the proton momenta, the pion
             rapidities and transverse momenta, and the pion–pion
             invariant mass. Cross-section values of 4.8±1.0(stat)-0.2+0.3(syst)μb
             and 9±6(stat)-2+2(syst)μb are obtained in the two regions;
             they are compared with theoretical models and provide a
             demonstration of the feasibility of measurements of this
             type.},
   Doi = {10.1140/epjc/s10052-023-11700-x},
   Key = {fds371907}
}

@article{fds321114,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of exclusive γγ →w+W- production and search
             for exclusive Higgs boson production in pp collisions at s
             =8 TeV using the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.032011},
   Abstract = {Searches for exclusively produced W boson pairs in the
             process pp(γγ)→pW+W-p and an exclusively produced Higgs
             boson in the process pp(gg)→pHp have been performed using
             e±μ final states. These measurements use 20.2 fb-1 of pp
             collisions collected by the ATLAS experiment at a
             center-of-mass energy s=8 TeV at the LHC. Exclusive
             production of W+W- consistent with the Standard Model
             prediction is found with 3.0σ significance. The exclusive
             W+W- production cross section is determined to be
             σ(γγ→W+W-→e±μX)=6.9±2.2(stat)±1.4(sys) fb, in
             agreement with the Standard Model prediction. Limits on
             anomalous quartic gauge couplings are set at 95% confidence
             level as -1.7×10-6<a0W/Λ2<1.7×10-6 GeV-2 and
             -6.4×10-6<aCW/Λ2<6.3×10-6 GeV-2. A 95% confidence-level
             upper limit on the total production cross section for an
             exclusive Higgs boson is set to 1.2 pb.},
   Doi = {10.1103/PhysRevD.94.032011},
   Key = {fds321114}
}

@article{fds310259,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of exclusive γγ→ℓ+
             production in proton–proton collisions at √s=7 TeV with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {749},
   Pages = {242-261},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.07.069},
   Abstract = {This Letter reports a measurement of the exclusive
             γγ→ℓ+ℓ− (ℓ=e, μ) cross-section in
             proton–proton collisions at a centre-of-mass energy of 7
             TeV by the ATLAS experiment at the LHC, based on an
             integrated luminosity of 4.6 fb−1. For the electron or
             muon pairs satisfying exclusive selection criteria, a fit to
             the dilepton acoplanarity distribution is used to extract
             the fiducial cross-sections. The cross-section in the
             electron channel is determined to be σγγ→e+e−excl.=0.428
             ± 0.035 (stat.) ± 0.018 (syst.) pb for a phase–space
             region with invariant mass of the electron pairs greater
             than 24 GeV, in which both electrons have transverse
             momentum pT>12 GeV and pseudorapidity |η|<2.4. For muon
             pairs with invariant mass greater than 20 GeV, muon
             transverse momentum pT>10 GeV and pseudorapidity |η|<2.4,
             the cross-section is determined to be σγγ→μ+μ−excl.=0.628
             ± 0.032 (stat.) ± 0.021 (syst.) pb. When proton absorptive
             effects due to the finite size of the proton are taken into
             account in the theory calculation, the measured
             cross-sections are found to be consistent with the theory
             prediction.},
   Doi = {10.1016/j.physletb.2015.07.069},
   Key = {fds310259}
}

@article{fds356568,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud,
             AA and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob,
             M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Estevez, MA and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
             JAA and Bella, LA and Arabidze, G},
   Title = {Measurement of fiducial and differential
             W+W- production cross-sections at
             √s=13 TeV with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {10},
   Year = {2019},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7371-6},
   Abstract = {A measurement of fiducial and differential cross-sections
             for W+W- production in proton–proton collisions at
             s=13 TeV with the ATLAS experiment at the Large Hadron
             Collider using data corresponding to an integrated
             luminosity of 36.1 fb - 1 is presented. Events with one
             electron and one muon are selected, corresponding to the
             decay of the diboson system as WW→ e±νμ∓ν. To
             suppress top-quark background, events containing jets with a
             transverse momentum exceeding 35 GeV are not included in
             the measurement phase space. The fiducial cross-section, six
             differential distributions and the cross-section as a
             function of the jet-veto transverse momentum threshold are
             measured and compared with several theoretical predictions.
             Constraints on anomalous electroweak gauge boson
             self-interactions are also presented in the framework of a
             dimension-six effective field theory.},
   Doi = {10.1140/epjc/s10052-019-7371-6},
   Key = {fds356568}
}

@article{fds321107,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Measurement of fiducial differential cross sections of
             gluon-fusion production of Higgs bosons decaying to WW
             →eνμν with the ATLAS detector at √s=8
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2016)104},
   Abstract = {This paper describes a measurement of fiducial and
             differential cross sections of gluon-fusion Higgs boson
             production in the H → W W∗→ eνμν channel, using
             20.3 fb−1 of proton-proton collision data. The data were
             produced at a centre-of-mass energy of s=8 TeV at the CERN
             Large Hadron Collider and recorded by the ATLAS detector in
             2012. Cross sections are measured from the observed H→ W
             W∗→ eνμν signal yield in categories distinguished by
             the number of associated jets. The total cross section is
             measured in a fiducial region defined by the kinematic
             properties of the charged leptons and neutrinos.
             Differential cross sections are reported as a function of
             the number of jets, the Higgs boson transverse momentum, the
             dilepton rapidity, and the transverse momentum of the
             leading jet. The jet-veto efficiency, or fraction of events
             with no jets above a given transverse momentum threshold, is
             also reported. All measurements are compared to QCD
             predictions from Monte Carlo generators and fixed-order
             calculations, and are in agreement with the Standard Model
             predictions.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP08(2016)104},
   Key = {fds321107}
}

@article{fds356555,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
             JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
             VA},
   Title = {Measurement of flow harmonics correlations with mean
             transverse momentum in lead–lead and proton–lead
             collisions at √sNN=5.02TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {12},
   Year = {2019},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7489-6},
   Abstract = {To assess the properties of the quark–gluon plasma formed
             in ultrarelativistic ion collisions, the ATLAS experiment at
             the LHC measures a correlation between the mean transverse
             momentum and the flow harmonics. The analysis uses data
             samples of lead–lead and proton–lead collisions obtained
             at the centre-of-mass energy per nucleon pair of 5.02 TeV,
             corresponding to total integrated luminosities of 22μb-1
             and 28nb-1, respectively. The measurement is performed using
             a modified Pearson correlation coefficient with the
             charged-particle tracks on an event-by-event basis. The
             modified Pearson correlation coefficients for the 2nd-,
             3rd-, and 4th-order flow harmonics are measured in the
             lead–lead collisions as a function of event centrality
             quantified as the number of charged particles or the number
             of nucleons participating in the collision. The measurements
             are performed for several intervals of the charged-particle
             transverse momentum. The correlation coefficients for all
             studied harmonics exhibit a strong centrality evolution,
             which only weakly depends on the charged-particle momentum
             range. In the proton–lead collisions, the modified Pearson
             correlation coefficient measured for the 2nd-order flow
             harmonics shows only weak centrality dependence. The
             lead-lead data is qualitatively described by the predictions
             based on the hydrodynamical model.},
   Doi = {10.1140/epjc/s10052-019-7489-6},
   Key = {fds356555}
}

@article{fds313588,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Measurement of flow harmonics with multi-particle cumulants
             in Pb+Pb collisions at [Formula: see text] TeV with the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {11},
   Pages = {3157},
   Year = {2014},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3157-z},
   Abstract = {ATLAS measurements of the azimuthal anisotropy in lead-lead
             collisions at [Formula: see text] TeV are shown using a
             dataset of approximately 7 [Formula: see text]b[Formula:
             see text] collected at the LHC in 2010. The measurements are
             performed for charged particles with transverse momenta
             [Formula: see text] GeV and in the pseudorapidity range
             [Formula: see text]. The anisotropy is characterized by the
             Fourier coefficients, [Formula: see text], of the
             charged-particle azimuthal angle distribution for [Formula:
             see text]-4. The Fourier coefficients are evaluated using
             multi-particle cumulants calculated with the generating
             function method. Results on the transverse momentum,
             pseudorapidity and centrality dependence of the [Formula:
             see text] coefficients are presented. The elliptic flow,
             [Formula: see text], is obtained from the two-, four-, six-
             and eight-particle cumulants while higher-order
             coefficients, [Formula: see text] and [Formula: see text],
             are determined with two- and four-particle cumulants. Flow
             harmonics [Formula: see text] measured with four-particle
             cumulants are significantly reduced compared to the
             measurement involving two-particle cumulants. A comparison
             to [Formula: see text] measurements obtained using different
             analysis methods and previously reported by the LHC
             experiments is also shown. Results of measurements of flow
             fluctuations evaluated with multi-particle cumulants are
             shown as a function of transverse momentum and the collision
             centrality. Models of the initial spatial geometry and its
             fluctuations fail to describe the flow fluctuations
             measurements.},
   Doi = {10.1140/epjc/s10052-014-3157-z},
   Key = {fds313588}
}

@article{fds356749,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of forward-backward multiplicity correlations in
             lead-lead, proton-lead, and proton-proton collisions with
             the ATLAS detector},
   Journal = {Physical Review C},
   Volume = {95},
   Number = {6},
   Year = {2017},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevC.95.064914},
   Abstract = {Two-particle pseudorapidity correlations are measured in
             sNN=2.76TeVPb+Pb, sNN=5.02TeVp+Pb, and s=13TeVpp collisions
             at the Large Hadron Collider (LHC), with total integrated
             luminosities of approximately 7μb-1, 28 nb-1, and 65 nb-1,
             respectively. The correlation function CN(η1,η2) is
             measured as a function of event multiplicity using charged
             particles in the pseudorapidity range |η|<2.4. The
             correlation function contains a significant short-range
             component, which is estimated and subtracted. After removal
             of the short-range component, the shape of the correlation
             function is described approximately by 1+(a12)1/2η1η2 in
             all collision systems over the full multiplicity range. The
             values of (a12)1/2 are consistent for the opposite-charge
             pairs and same-charge pairs, and for the three collision
             systems at similar multiplicity. The values of (a12)1/2 and
             the magnitude of the short-range component both follow a
             power-law dependence on the event multiplicity. The
             short-range component in p + Pb collisions, after
             symmetrizing the proton and lead directions, is found to be
             smaller at a given η than in pp collisions with comparable
             multiplicity.},
   Doi = {10.1103/PhysRevC.95.064914},
   Key = {fds356749}
}

@article{fds313615,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Measurement of four-jet differential cross sections in
             √s=8 TeV proton-proton collisions using the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {12},
   Pages = {1-76},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2015)105},
   Abstract = {Differential cross sections for the production of at least
             four jets have been measured in proton-proton collisions at
             (Formula presented.) TeV at the Large Hadron Collider using
             the ATLAS detector. Events are selected if the four anti-ktR
             = 0.4 jets with the largest transverse momentum (pT) within
             the rapidity range |y| < 2.8 are well separated (ΔR4jmin >
             0.65), all have pT > 64 GeV, and include at least one jet
             with pT > 100 GeV. The dataset corresponds to an integrated
             luminosity of 20.3 fb−1. The cross sections, corrected for
             detector effects, are compared to leading-order and
             next-to-leading-order calculations as a function of the jet
             momenta, invariant masses, minimum and maximum opening
             angles and other kinematic variables.},
   Doi = {10.1007/JHEP12(2015)105},
   Key = {fds313615}
}

@article{fds355146,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R},
   Title = {Measurement of hadronic event shapes in high-p T
             multijet final states at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {1},
   Year = {2021},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2021)188},
   Abstract = {A measurement of event-shape variables in proton-proton
             collisions at large momentum transfer is presented using
             data collected at s = 13 TeV with the ATLAS detector at the
             Large Hadron Collider. Six event-shape variables calculated
             using hadronic jets are studied in inclusive multijet events
             using data corresponding to an integrated luminosity of 139
             fb−1. Measurements are performed in bins of jet
             multiplicity and in different ranges of the scalar sum of
             the transverse momenta of the two leading jets, reaching
             scales beyond 2 TeV. These measurements are compared with
             predictions from Monte Carlo event generators containing
             leading-order or next-to-leading order matrix elements
             matched to parton showers simulated to leading-logarithm
             accuracy. At low jet multiplicities, shape discrepancies
             between the measurements and the Monte Carlo predictions are
             observed. At high jet multiplicities, the shapes are better
             described but discrepancies in the normalisation are
             observed. [Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP01(2021)188},
   Key = {fds355146}
}

@article{fds317295,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Ochoa, MI and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Measurement of hard double-parton interactions in W(→ lν)
             + 2-jet events at √s = 7 TeV with the ATLAS
             detector},
   Journal = {New Journal of Physics},
   Volume = {15},
   Number = {3},
   Pages = {033038-033038},
   Publisher = {IOP Publishing},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1088/1367-2630/15/3/033038},
   Abstract = {The production of W bosons in association with two jets in
             proton-proton collisions at a centre-of-mass energy of √ s
             = 7 TeV has been analysed for the presence of double-parton
             interactions using data corresponding to an integrated
             luminosity of 36 pb-1, collected with the ATLAS detector at
             the Large Hadron Collider. The fraction of events arising
             from double-parton interactions, f(D)DP, has been measured
             through the pT balance between the two jets and amounts to
             f(D)DP = 0.08 ±0.01 (stat.)±0.02 (sys.) for jets with
             transverse momentum pT > 20 GeV and rapidity |y| < 2.8. This
             corresponds to a measurement of the effective area parameter
             for hard double-parton interactions of σeff = 15 ± 3
             (stat.) +5-3 (sys.) mb.},
   Doi = {10.1088/1367-2630/15/3/033038},
   Key = {fds317295}
}

@article{fds310340,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H},
   Title = {Measurement of Higgs boson production in the diphoton decay
             channel in pp collisions at center-of-mass energies of 7 and
             8 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.112015},
   Abstract = {A measurement of the production processes of the recently
             discovered Higgs boson is performed in the two-photon final
             state using 4.5 fb-1of proton-proton collisions data at √s
             = 7 TeV and 20.3 fb-1at √s = 8 TeV collected by the ATLAS
             detector at the Large Hadron Collider. The number of
             observed Higgs boson decays to diphotons divided by the
             corresponding Standard Model prediction, called the signal
             strength, is found to be μ = 1.17 ± 0.27 at the value of
             the Higgs boson mass measured by ATLAS, mH= 125.4 GeV. The
             analysis is optimized to measure the signal strengths for
             individual Higgs boson production processes at this value of
             mH. They are found to be μggF= 1.32 ± 0.38, μVBF= 0.8 ±
             0.7, μWH= 1.0 ± 1.6, μZH= 0.1+3.7-0.1, and μtt¯H=
             1.6+2.7-1.8, for Higgs boson production through gluon
             fusion, vector-boson fusion, and in association with a W or
             Z boson or a top-quark pair, respectively. Compared with the
             previously published ATLAS analysis, the results reported
             here also benefit from a new energy calibration procedure
             for photons and the subsequent reduction of the systematic
             uncertainty on the diphoton mass resolution. No significant
             deviations from the predictions of the Standard Model are
             found.},
   Doi = {10.1103/PhysRevD.90.112015},
   Key = {fds310340}
}

@article{fds329966,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Measurement of inclusive and differential cross sections in
             the H → ZZ * → 4ℓ decay channel in pp
             collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2017},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2017)132},
   Abstract = {Inclusive and differential fiducial cross sections of Higgs
             boson production in proton-proton collisions are measured in
             the H → ZZ* → 4ℓ decay channel. The proton-proton
             collision data were produced at the Large Hadron Collider at
             a centre-of-mass energy of 13 TeV and recorded by the ATLAS
             detector in 2015 and 2016, corresponding to an integrated
             luminosity of 36.1 fb−1. The inclusive fiducial cross
             section in the H → ZZ* → 4ℓ decay channel is measured
             to be 3.62 ± 0.50(stat)− 0.20+ 0.25 (sys) fb, in
             agreement with the Standard Model prediction of 2.91 ± 0.13
             fb. The cross section is also extrapolated to the total
             phase space including all Standard Model Higgs boson decays.
             Several differential fiducial cross sections are measured
             for observables sensitive to the Higgs boson production and
             decay, including kinematic distributions of jets produced in
             association with the Higgs boson. Good agreement is found
             between data and Standard Model predictions. The results are
             used to put constraints on anomalous Higgs boson
             interactions with Standard Model particles, using the
             pseudo-observable extension to the kappa-framework.[Figure
             not available: see fulltext.].},
   Doi = {10.1007/JHEP10(2017)132},
   Key = {fds329966}
}

@article{fds308138,
   Author = {Abazov, VM and Abbott, B and Abolins, M and Acharya, BS and Adams, M and Adams, T and Agelou, M and Agram, J-L and Ahn, SH and Ahsan, M and Alexeev,
             GD and Alkhazov, G and Alton, A and Alverson, G and Alves, GA and Anastasoaie, M and Andeen, T and Anderson, S and Andrieu, B and Arnoud,
             Y and Askew, A and Asman, B and Assis Jesus and ACS and Atramentov, O and Autermann, C and Avila, C and Badaud, F and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Bargassa, P and Baringer,
             P and Barnes, C and Barreto, J and Bartlett, JF and Bassler, U and Bauer,
             D and Bean, A and Beauceron, S and Begel, M and Bellavance, A and Beri, SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Binder,
             M and Biscarat, C and Black, KM and Blackler, I and Blazey, G and Blekman,
             F and Blessing, S and Bloch, D and Blumenschein, U and Boehnlein, A and Boeriu, O and Bolton, TA and Borcherding, F and Borissov, G and Bos, K and Bose, T and Brandt, A and Brock, R and Brooijmans, G and Bross, A and Buchanan, NJ and Buchholz, D and Buehler, M and Buescher, V and Burdin,
             S and Burnett, TH and Busato, E and Butler, JM and Bystricky, J and Caron,
             S and Carvalho, W and Casey, BCK and Cason, NM and Castilla-Valdez, H and Chakrabarti, S and Chakraborty, D and Chan, KM and Chandra, A and Chapin, D and Charles, F and Cheu, E and Cho, DK and Choi, S and Choudhary,
             B and Christiansen, T and Christofek, L and Claes, D and Clément, B and Clément, C and Coadou, Y and Cooke, M and Cooper, WE and Coppage, D and Corcoran, M and Cothenet, A and Cousinou, M-C and Cox, B and Crépé-Renaudin, S and Cristetiu, M and Cutts, D and da Motta, H and Davies, B and Davies, G and Davis, GA and De, K and de Jong, P and de Jong,
             SJ and De La Cruz-Burelo and E and De Oliveira Martins and C and Dean, S and Degenhardt, JD and Déliot, F and Demarteau, M and Demina, R and Demine,
             P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg,
             M and Doidge, M and Dong, H and Doulas, S and Dudko, LV and Duflot, L and Dugad, SR and Duperrin, A and Dyer, J and Dyshkant, A and Eads, M and Edmunds, D and Edwards, T and Ellison, J and Elmsheuser, J and Elvira,
             VD and Eno, S and Ermolov, P and Eroshin, OV and Estrada, J and Evans, D and Evans, H and Evdokimov, A and Evdokimov, VN and Fast, J and Fatakia, SN and Feligioni, L and Ferbel, T and Fiedler, F and Filthaut, F and Fisher, W and Fisk, HE and Fleck, I and Fortner, M and Fox, H and Fu, S and Fuess, S and Gadfort, T and Galea, CF and Gallas, E and Galyaev, E and Garcia, C and Garcia-Bellido, A and Gardner, J and Gavrilov, V and Gay, P and Gelé,
             D and Gelhaus, R and Genser, K and Gerber, CE and Gershtein, Y and Ginther,
             G and Golling, T and Gómez, B and Gounder, K and Goussiou, A and Grannis,
             PD and Greder, S and Greenlee, H and Greenwood, ZD and Gregores, EM and Gris, P and Grivaz, J-F and Groer, L and Grünendahl, S and Grünewald,
             MW and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Haas, A and Hadley, NJ and Hagopian, S and Hall, I and Hall, RE and Han, C and Han, L and Hanagaki, K and Harder, K and Harrington, R and Hauptman, JM and Hauser,
             R and Hays, J and Hebbeker, T and Hedin, D and Heinmiller, JM and Heinson,
             AP and Heintz, U and Hensel, C and Hesketh, G and Hildreth, MD and Hirosky,
             R and Hobbs, JD and Hoeneisen, B and Hohlfeld, M and Hong, SJ and Hooper,
             R and Houben, P and Hu, Y and Huang, J and Iashvili, I and Illingworth, R and Ito, AS and Jabeen, S and Jaffré, M and Jain, S and Jain, V and Jakobs, K and Jenkins, A and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jonsson, P and Juste, A and Käfer, D and Kahl, W and Kahn, S and Kajfasz,
             E and Kalinin, AM and Kalk, J and Karmanov, D and Kasper, J and Kau, D and Kaur, R and Kehoe, R and Kermiche, S and Kesisoglou, S and Khanov, A and Kharchilava, A and Kharzheev, YM and Kim, H and Klima, B and Klute, M and Kohli, JM and Kopal, M and Korablev, VM and Kotcher, J and Kothari, B and Koubarovsky, A and Kozelov, AV and Kozminski, J and Kryemadhi, A and Krzywdzinski, S and Kuleshov, S and Kulik, Y and Kumar, A and Kunori, S and Kupco, A and Kurca, T and Kvita, J and Lager, S and Lahrichi, N and Landsberg, G and Lazoflores, J and Le Bihan and A-C and Lebrun, P and Lee,
             WM and Leflat, A and Lehner, F and Leonidopoulos, C and Leveque, J and Lewis, P and Li, J and Li, QZ and Lima, JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipaev, VV and Lipton, R and Lobo, L and Lobodenko, A and Lokajicek, M and Lounis, A and Love, P and Lubatti, HJ and Lueking, L and Lynker, M and Lyon, AL and Maciel, AKA and Madaras, RJ and Mättig, P and Magass, C and Magerkurth, A and Magnan, A-M and Makovec, N and Mal, PK and Malbouisson, HB and Malik, S and Malyshev, VL and Mao, HS and Maravin,
             Y and Martens, M and Mattingly, SEK and Mayorov, AA and McCarthy, R and McCroskey, R and Meder, D and Melanson, HL and Melnitchouk, A and Mendes, A and Merkin, M and Merritt, KW and Meyer, A and Michaut, M and Miettinen, H and Mitrevski, J and Mokhov, N and Molina, J and Mondal,
             NK and Moore, RW and Muanza, GS and Mulders, M and Mutaf, YD and Nagy, E and Narain, M and Naumann, NA and Neal, HA and Negret, JP and Nelson, S and Neustroev, P and Noeding, C and Nomerotski, A and Novaes, SF and Nunnemann, T and Nurse, E and O'Dell, V and O'Neil, DC and Oguri, V and Oliveira, N and Oshima, N and Otero y Garzón and GJ and Padley, P and Parashar, N and Park, SK and Parsons, J and Partridge, R and Parua, N and Patwa, A and Perea, PM and Perez, E and Pétroff, P and Petteni, M and Phaf, L and Piegaia, R and Pleier, M-A and Podesta-Lerma, PLM and Podstavkov, VM and Pogorelov, Y and Pope, BG and Silva, WLPD and Prosper, HB and Protopopescu, S and Qian, J and Quadt, A and Quinn, B and Rani, KJ and Ranjan, K and Rapidis, PA and Ratoff, PN and Reay, NW and Reucroft, S and Rijssenbeek, M and Ripp-Baudot, I and Rizatdinova, F and Rodrigues, RF and Royon, C and Rubinov, P and Ruchti, R and Rud, VI and Sajot, G and Sánchez-Hernández, A and Sanders, MP and Santoro, A and Savage, G and Sawyer, L and Scanlon, T and Schaile, D and Schamberger,
             RD and Schellman, H and Schieferdecker, P and Schmitt, C and Schwartzman, A and Schwienhorst, R and Sengupta, S and Severini, H and Shabalina, E and Shamim, M and Shary, V and Shchukin, AA and Shephard,
             WD and Shivpuri, RK and Shpakov, D and Sidwell, RA and Simak, V and Sirotenko, V and Skubic, P and Slattery, P and Smith, RP and Smolek, K and Snow, GR and Snow, J and Snyder, S and Söldner-Rembold, S and Song, X and Sonnenschein, L and Sopczak, A and Sosebee, M and Soustruznik, K and Souza, M and Spurlock, B and Stanton, NR and Stark, J and Steele, J and Stevenson, K and Stolin, V and Stone, A and Stoyanova, DA and Strandberg, J and Strang, MA and Strauss, M and Ströhmer, R and Strom,
             D and Strovink, M and Stutte, L and Sumowidagdo, S and Sznajder, A and Talby, M and Tamburello, P and Taylor, W and Telford, P and Temple, J and Thomas, E and Thooris, B and Tomoto, M and Toole, T and Torborg, J and Towers, S and Trefzger, T and Trincaz-Duvoid, S and Tuchming, B and Tully, C and Turcot, AS and Tuts, PM and Uvarov, L and Uvarov, S and Uzunyan, S and Vachon, B and Van Kooten and R and van Leeuwen, WM and Varelas, N and Varnes, EW and Vartapetian, A and Vasilyev, IA and Vaupel, M and Verdier, P and Vertogradov, LS and Verzocchi, M and Villeneuve-Seguier, F and Vlimant, J-R and Von Toerne and E and Vreeswijk, M and Vu, AT and Wahl, HD and Walker, R and Wang, L and Wang,
             Z-M and Warchol, J and Watts, G},
   Title = {Measurement of inclusive differential cross sections for pp
             collisions at (square root)s = 1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {94},
   Number = {23},
   Pages = {232001},
   Year = {2005},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.94.232001},
   Abstract = {We present measurements of the inclusive production cross
             sections of the Gamma(1S) bottomonium state in pp collisions
             at (square root)s = 1.96 TeV. Using the Gamma(1S) -->
             mu(+)mu(-) decay mode for a data sample of 159 +/- 10 pb(-1)
             collected by the D0 detector at the Fermilab Tevatron
             collider, we determine the differential cross sections as a
             function of the Gamma(1S) transverse momentum for three
             ranges of the Gamma(1S) rapidity: 0 < y(Gamma) < or = 0.6,
             0.6 < y(Gamma) < or = 1.2, and 1.2 < y(Gamma) < or =
             1.8.},
   Doi = {10.1103/physrevlett.94.232001},
   Key = {fds308138}
}

@article{fds356686,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Measurement of inclusive jet and dijet cross-sections in
             proton-proton collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {5},
   Year = {2018},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2018)195},
   Abstract = {Inclusive jet and dijet cross-sections are measured in
             proton-proton collisions at a centre-of-mass energy of 13
             TeV. The measurement uses a dataset with an integrated
             luminosity of 3.2 fb−1 recorded in 2015 with the ATLAS
             detector at the Large Hadron Collider. Jets are identified
             using the anti-kt algorithm with a radius parameter value of
             R = 0.4. The inclusive jet cross-sections are measured
             double-differentially as a function of the jet transverse
             momentum, covering the range from 100 GeV to 3.5 TeV, and
             the absolute jet rapidity up to |y| = 3. The
             double-differential dijet production cross-sections are
             presented as a function of the dijet mass, covering the
             range from 300 GeV to 9 TeV, and the half absolute rapidity
             separation between the two leading jets within |y| < 3,
             y∗, up to y∗ = 3. Next-to-leading-order, and
             next-to-next-to-leading-order for the inclusive jet
             measurement, perturbative QCD calculations corrected for
             non-perturbative and electroweak effects are compared to the
             measured cross-sections.},
   Doi = {10.1007/JHEP05(2018)195},
   Key = {fds356686}
}

@article{fds307747,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Aktas, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A},
   Title = {Measurement of inclusive jet and dijet production in pp
             collisions at √s=7TeV using the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.014022},
   Abstract = {Inclusive jet and dijet cross sections have been measured in
             proton-proton collisions at a center-of-mass energy of 7 TeV
             using the ATLAS detector at the Large Hadron Collider. The
             cross sections were measured using jets clustered with the
             anti-kt algorithm with parameters R=0.4 and R=0.6. These
             measurements are based on the 2010 data sample, consisting
             of a total integrated luminosity of 37pb-1. Inclusive jet
             double-differential cross sections are presented as a
             function of jet transverse momentum, in bins of jet
             rapidity. Dijet double-differential cross sections are
             studied as a function of the dijet invariant mass, in bins
             of half the rapidity separation of the two leading jets. The
             measurements are performed in the jet rapidity range
             |y|<4.4, covering jet transverse momenta from 20 GeV to 1.5
             TeV and dijet invariant masses from 70 GeV to 5 TeV. The
             data are compared to expectations based on
             next-to-leading-order QCD calculations corrected for
             nonperturbative effects, as well as to next-to-leading-order
             Monte Carlo predictions. In addition to a test of the theory
             in a new kinematic regime, the data also provide sensitivity
             to parton distribution functions in a region where they are
             currently not well-constrained. © 2012 CERN. Published by
             the American Physical Society under the terms of the
             http://creativecommons.org/licenses/by/ 3.0/ Creative
             Commons Attribution 3.0 License. Further distribution of
             this work must maintain attribution to the author(s) and the
             published article's title, journal citation, and
             DOI.},
   Doi = {10.1103/PhysRevD.86.014022},
   Key = {fds307747}
}

@article{fds313587,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurement of inclusive jet charged-particle fragmentation
             functions in Pb+Pb collisions at √sNN=2.76 TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {739},
   Pages = {320-342},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {December},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.10.065},
   Abstract = {Measurements of charged-particle fragmentation functions of
             jets produced in ultra-relativistic nuclear collisions can
             provide insight into the modification of parton showers in
             the hot, dense medium created in the collisions. ATLAS has
             measured jets in sNN=2.76 TeV Pb+Pb collisions at the LHC
             using a data set recorded in 2011 with an integrated
             luminosity of 0.14 nb−1. Jets were reconstructed using the
             anti-kt algorithm with distance parameter values
             R=0.2,0.3,and 0.4. Distributions of charged-particle
             transverse momentum and longitudinal momentum fraction are
             reported for seven bins in collision centrality for R=0.4
             jets with pTjet>100 GeV. Commensurate minimum pT values are
             used for the other radii. Ratios of fragment distributions
             in each centrality bin to those measured in the most
             peripheral bin are presented. These ratios show a reduction
             of fragment yield in central collisions relative to
             peripheral collisions at intermediate z values,
             0.04≲z≲0.2, and an enhancement in fragment yield for
             z≲0.04. A smaller, less significant enhancement is
             observed at large z and large pT in central
             collisions.},
   Doi = {10.1016/j.physletb.2014.10.065},
   Key = {fds313587}
}

@article{fds310406,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of inclusive two-particle angular correlations
             in pp collisions with the atlas detector at the
             LHC},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP05(2012)157},
   Abstract = {We present a measurement of two-particle angular
             correlations in protonproton collisions at √a = 900 GeV
             and 7TeV. The collision events were collected during 2009
             and 2010 with the ATLAS detector at the Large Hadron
             Collider using a single-arm minimum bias trigger.
             Correlations are measured for charged particles produced in
             the kinematic range of transverse momentum pT > 100MeV and
             pseudorapidity |n| < 2.5. A complex structure in
             pseudorapidity and azimuth is observed at both collision
             energies. Results are compared to pythia 8 and herwig++ as
             well as to the AMBT2B, DW and Perugia 2011 tunes of pythia
             6. The data are not satisfactorily described by any of these
             models.},
   Doi = {10.1007/JHEP05(2012)157},
   Key = {fds310406}
}

@article{fds310341,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Measurement of indirect CP -violating asymmetries in D0
             →k+K- and D0 →π+π- decays at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.111103},
   Abstract = {We report a measurement of the indirect CP-violating
             asymmetries (AΓ) between effective lifetimes of anticharm
             and charm mesons reconstructed in D0→K+K- and D0→π+π-
             decays. We use the full data set of proton-antiproton
             collisions collected by the Collider Detector at Fermilab
             experiment and corresponding to 9.7fb-1 of integrated
             luminosity. The strong-interaction decay D∗+→D0π+ is
             used to identify the meson at production as D0 or D¯0. We
             statistically subtract D0 and D¯0 mesons originating from
             b-hadron decays and measure the yield asymmetry between
             anticharm and charm decays as a function of decay time. We
             measure AΓ(K+K-)=(-0.19±0.15(stat)±0.04(syst))% and
             AΓ(π+π-)=(-0.01±0.18(stat)±0.03(syst))%. The results
             are consistent with the hypothesis of CP symmetry and their
             combination yields AΓ=(-0.12±0.12)%.},
   Doi = {10.1103/PhysRevD.90.111103},
   Key = {fds310341}
}

@article{fds307645,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Measurement of isolated-photon pair production in pp
             collisions at √s=7TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2013)086},
   Abstract = {The ATLAS experiment at the LHC has measured the production
             cross section of events with two isolated photons in the
             final state, in proton-proton collisions at √s=7TeV . The
             full data set collected in 2011, corresponding to an
             integrated luminosity of 4.9 fb-1, is used. The amount of
             background, from hadronic jets and isolated electrons, is
             estimated with data-driven techniques and subtracted. The
             total cross section, for two isolated photons with
             transverse energies above 25 GeV and 22 GeV respectively, in
             the acceptance of the electromagnetic calorimeter (|η| <
             1.37 and 1.52 < |η| < 2.37) and with an angular separation
             ΔR > 0.4, is 44.0-4.2+3.2 pb. The differential cross
             sections as a function of the di-photon invariant mass,
             transverse momentum, azimuthal separation, and cosine of the
             polar angle of the largest transverse energy photon in the
             Collins-Soper di-photon rest frame are also measured. The
             results are compared to the prediction of leading-order
             parton-shower and next-to-leading-order and
             next-to-next-to-leading-order parton-level
             generators.[Figure not available: see fulltext.] © 2013
             CERN for the benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP01(2013)086},
   Key = {fds307645}
}

@article{fds349433,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
             Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP},
   Title = {Measurement of isolated-photon plus two-jet production in pp
             collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {3},
   Year = {2020},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2020)179},
   Abstract = {The dynamics of isolated-photon plus two-jet production in
             pp collisions at a centre-of-mass energy of 13 TeV are
             studied with the ATLAS detector at the LHC using a dataset
             corresponding to an integrated luminosity of 36.1 fb−1.
             Cross sections are measured as functions of a variety of
             observables, including angular correlations and invariant
             masses of the objects in the final state, γ + jet + jet.
             Measurements are also performed in phase-space regions
             enriched in each of the two underlying physical mechanisms,
             namely direct and fragmentation processes. The measurements
             cover the range of photon (jet) transverse momenta from 150
             GeV (100 GeV) to 2 TeV. The tree-level plus parton-shower
             predictions from Sherpa and Pythia as well as the
             next-to-leading-order QCD predictions from Sherpa are
             compared with the measurements. The next-to-leading-order
             QCD predictions describe the data adequately in shape and
             normalisation except for regions of phase space such as
             those with high values of the invariant mass or rapidity
             separation of the two jets, where the predictions
             overestimate the data. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP03(2020)179},
   Key = {fds349433}
}

@article{fds356550,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Arduh, FA and Arguin,
             JF},
   Title = {Measurement of J/ψ production in association with a W
             ± boson with pp data at 8 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {1},
   Year = {2020},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2020)095},
   Abstract = {A measurement of the production of a prompt J/ψ meson in
             association with a W± boson with W± → μν and J/ψ →
             μ+μ− is presented for J/ψ transverse momenta in the
             range 8.5–150 GeV and rapidity |yJ/ψ| < 2.1 using ATLAS
             data recorded in 2012 at the LHC. The data were taken at a
             proton-proton centre-of-mass energy of s = 8 TeV and
             correspond to an integrated luminosity of 20.3 fb−1. The
             ratio of the prompt J/ψ plus W± cross-section to the
             inclusive W± cross-section is presented as a differential
             measurement as a function of J/ψ transverse momenta and
             compared with theoretical predictions using different
             double-parton-scattering cross-sections. [Figure not
             available: see fulltext.].},
   Doi = {10.1007/JHEP01(2020)095},
   Key = {fds356550}
}

@article{fds321095,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Measurement of jet activity in top quark events using the
             eμ final state with two b-tagged jets in pp collisions at
             √s=8 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2016)074},
   Abstract = {Measurements of the jet activity in tt¯ events produced in
             proton-proton collisions at s=8 TeV are presented, using
             20.3 fb−1 of data collected by the ATLAS experiment at the
             Large Hadron Collider. The events were selected in the
             dilepton eμ decay channel with two identified b-jets. The
             numbers of additional jets for various jet transverse
             momentum (pT) thresholds, and the normalised differential
             cross-sections as a function of pT for the five highest-pT
             additional jets, were measured in the jet pseudo-rapidity
             range |η| < 4.5. The gap fraction, the fraction of events
             which do not contain an additional jet in a central rapidity
             region, was measured for several rapidity intervals as a
             function of the minimum pT of a single jet or the scalar sum
             of pT of all additional jets. These fractions were also
             measured in different intervals of the invariant mass of the
             eμbb¯ system. All measurements were corrected for detector
             effects, and found to be mostly well-described by
             predictions from next-to-leading-order and leading-order
             tt¯ event generators with appropriate parameter choices.
             The results can be used to further optimise the parameters
             used in such generators.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP09(2016)074},
   Key = {fds321095}
}

@article{fds347497,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
             H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Bell,
             AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
             J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer,
             F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin,
             S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke,
             S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
             S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda,
             E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro,
             NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez
             Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
             S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
   Title = {Measurement of jet activity produced in top-quark events
             with an electron, a muon and two b-tagged jets in the
             final state in pp collisions at [Formula: see text]
             TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {4},
   Pages = {220},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4766-0},
   Abstract = {Measurements of jet activity in top-quark pair events
             produced in proton-proton collisions are presented, using
             3.2 fb[Formula: see text] of <i>pp</i> collision data at a
             centre-of-mass energy of 13 TeV collected by the ATLAS
             experiment at the Large Hadron Collider. Events are chosen
             by requiring an opposite-charge [Formula: see text] pair and
             two <i>b</i>-tagged jets in the final state. The normalised
             differential cross-sections of top-quark pair production are
             presented as functions of additional-jet multiplicity and
             transverse momentum, [Formula: see text]. The fraction of
             signal events that do not contain additional jet activity in
             a given rapidity region, the gap fraction, is measured as a
             function of the [Formula: see text] threshold for additional
             jets, and is also presented for different invariant mass
             regions of the [Formula: see text] system. All measurements
             are corrected for detector effects and presented as
             particle-level distributions compared to predictions with
             different theoretical approaches for QCD radiation. While
             the kinematics of the jets from top-quark decays are
             described well, the generators show differing levels of
             agreement with the measurements of observables that depend
             on the production of additional jets.},
   Doi = {10.1140/epjc/s10052-017-4766-0},
   Key = {fds347497}
}

@article{fds356779,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Measurement of jet charge in dijet events from s =8 TeV pp
             collisions with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {5},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.052003},
   Abstract = {The momentum-weighted sum of the charges of tracks
             associated to a jet is sensitive to the charge of the
             initiating quark or gluon. This paper presents a measurement
             of the distribution of momentum-weighted sums, called jet
             charge, in dijet events using 20.3 fb-1 of data recorded
             with the ATLAS detector at s=8 TeV in pp collisions at the
             LHC. The jet charge distribution is unfolded to remove
             distortions from detector effects and the resulting
             particle-level distribution is compared with several models.
             The pT dependence of the jet charge distribution average and
             standard deviation are compared to predictions obtained with
             several leading-order and next-to-leading-order parton
             distribution functions. The data are also compared to
             different Monte Carlo simulations of QCD dijet production
             using various settings of the free parameters within these
             models. The chosen value of the strong coupling constant
             used to calculate gluon radiation is found to have a
             significant impact on the predicted jet charge. There is
             evidence for a pT dependence of the jet charge distribution
             for a given jet flavor. In agreement with perturbative QCD
             predictions, the data show that the average jet charge of
             quark-initiated jets decreases in magnitude as the energy of
             the jet increases.},
   Doi = {10.1103/PhysRevD.93.052003},
   Key = {fds356779}
}

@article{fds356653,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold,
             H},
   Title = {Measurement of jet fragmentation in 5.02 TeV proton–lead
             and proton–proton collisions with the ATLAS
             detector},
   Journal = {Nuclear Physics A},
   Volume = {978},
   Pages = {65-106},
   Year = {2018},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.nuclphysa.2018.07.006},
   Abstract = {A measurement of the fragmentation functions of jets into
             charged particles in p+Pb collisions and pp collisions is
             presented. The analysis utilizes 28 nb−1 of p+Pb data and
             26 pb−1 of pp data, both at sNN= 5.02 TeV, collected in
             2013 and 2015, respectively, with the ATLAS detector at the
             LHC. The measurement is reported in the centre-of-mass frame
             of the nucleon–nucleon system for jets in the rapidity
             range |y⁎|<1.6 and with transverse momentum 45 <pT< 260
             GeV. Results are presented both as a function of the
             charged-particle transverse momentum and as a function of
             the longitudinal momentum fraction of the particle with
             respect to the jet. The pp fragmentation functions are
             compared with results from Monte Carlo event generators and
             two theoretical models. The ratios of the p+Pb to pp
             fragmentation functions are found to be consistent with
             unity.},
   Doi = {10.1016/j.nuclphysa.2018.07.006},
   Key = {fds356653}
}

@article{fds347502,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski,
             R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin,
             DL and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock,
             I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer,
             F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin,
             S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke,
             S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
             S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini,
             I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castelli, A and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ},
   Title = {Measurement of jet fragmentation in Pb+Pb and pp
             collisions at sNN=2.76 TeV with the ATLAS detector at the
             LHC.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {6},
   Pages = {379},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4915-5},
   Abstract = {The distributions of transverse momentum and longitudinal
             momentum fraction of charged particles in jets are measured
             in Pb+Pb and <i>pp</i> collisions with the ATLAS detector at
             the LHC. The distributions are measured as a function of jet
             transverse momentum and rapidity. The analysis utilises an
             integrated luminosity of 0.14 nb -1 of Pb+Pb data and 4.0 pb
             -1 of <i>pp</i> data collected in 2011 and 2013,
             respectively, at the same centre-of-mass energy of 2.76 TeV
             per colliding nucleon pair. The distributions measured in
             <i>pp</i> collisions are used as a reference for those
             measured in Pb+Pb collisions in order to evaluate the impact
             on the internal structure of jets from the jet energy loss
             of fast partons propagating through the hot, dense medium
             created in heavy-ion collisions. Modest but significant
             centrality-dependent modifications of fragmentation
             functions in Pb+Pb collisions with respect to those in
             <i>pp</i> collisions are seen. No significant dependence of
             modifications on jet pT and rapidity selections is observed
             except for the fragments with the highest transverse momenta
             for which some reduction of yields is observed for more
             forward jets.},
   Doi = {10.1140/epjc/s10052-017-4915-5},
   Key = {fds347502}
}

@article{fds356666,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
             Pereira, R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H},
   Title = {Measurement of jet fragmentation in Pb+Pb and pp collisions
             at sNN =5.02 TeV with the ATLAS detector},
   Journal = {Physical Review C},
   Volume = {98},
   Number = {2},
   Year = {2018},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevC.98.024908},
   Abstract = {This paper presents a measurement of jet fragmentation
             functions in 0.49 nb-1 of Pb+Pb collisions and 25 pb-1 of pp
             collisions at sNN=5.02 TeV collected in 2015 with the ATLAS
             detector at the LHC. These measurements provide insight into
             the jet quenching process in the quark-gluon plasma created
             in the aftermath of ultrarelativistic collisions between two
             nuclei. The modifications to the jet fragmentation functions
             are quantified by dividing the measurements in Pb+Pb
             collisions by baseline measurements in pp collisions. This
             ratio is studied as a function of the transverse momentum of
             the jet, the jet rapidity, and the centrality of the
             collision. In both collision systems, the jet fragmentation
             functions are measured for jets with transverse momentum
             between 126 and 398 GeV and with an absolute value of jet
             rapidity less than 2.1. An enhancement of particles carrying
             a small fraction of the jet momentum is observed, which
             increases with centrality and with increasing jet transverse
             momentum. Yields of particles carrying a very large fraction
             of the jet momentum are also observed to be enhanced.
             Between these two enhancements of the fragmentation
             functions a suppression of particles carrying an
             intermediate fraction of the jet momentum is observed in
             Pb+Pb collisions. A small dependence of the modifications on
             jet rapidity is observed.},
   Doi = {10.1103/PhysRevC.98.024908},
   Key = {fds356666}
}

@article{fds356724,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
             M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Measurement of jet pT correlations in Pb + Pb and
             pp collisions at sNN=2.76 TeVwith the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {774},
   Pages = {379-402},
   Year = {2017},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2017.09.078},
   Abstract = {Measurements of dijet pT correlations in Pb+Pb and pp
             collisions at a nucleon–nucleon centre-of-mass energy of
             sNN=2.76 TeV are presented. The measurements are performed
             with the ATLAS detector at the Large Hadron Collider using
             Pb+Pb and pp data samples corresponding to integrated
             luminosities of 0.14 nb−1 and 4.0 pb−1, respectively.
             Jets are reconstructed using the anti-kt algorithm with
             radius parameter values R=0.3 and R=0.4. A background
             subtraction procedure is applied to correct the jets for the
             large underlying event present in Pb+Pb collisions. The
             leading and sub-leading jet transverse momenta are denoted
             pT1 and pT2. An unfolding procedure is applied to the
             two-dimensional (pT1,pT2) distributions to account for
             experimental effects in the measurement of both jets.
             Distributions of (1/N)dN/dxJ, where xJ=pT2/pT1, are
             presented as a function of pT1 and collision centrality. The
             distributions are found to be similar in peripheral Pb+Pb
             collisions and pp collisions, but highly modified in central
             Pb+Pb collisions. Similar features are present in both the
             R=0.3 and R=0.4 results, indicating that the effects of the
             underlying event are properly accounted for in the
             measurement. The results are qualitatively consistent with
             expectations from partonic energy loss models.},
   Doi = {10.1016/j.physletb.2017.09.078},
   Key = {fds356724}
}

@article{fds307642,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
             P and Balli, F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
             DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
             R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat,
             P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
             M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley,
             AG and Buda, SI and Budagov, IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiarella,
             V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
             RN},
   Title = {Measurement of jet shapes in top-quark pair events at
             [Formula: see text] using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {12},
   Pages = {2676},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2676-3},
   Abstract = {A measurement of jet shapes in top-quark pair events using
             1.8 fb<sup>-1</sup> of [Formula: see text]<i>pp</i>
             collision data recorded by the ATLAS detector at the LHC is
             presented. Samples of top-quark pair events are selected in
             both the single-lepton and dilepton final states. The
             differential and integrated shapes of the jets initiated by
             bottom-quarks from the top-quark decays are compared with
             those of the jets originated by light-quarks from the
             hadronic <i>W</i>-boson decays [Formula: see text] in the
             single-lepton channel. The light-quark jets are found to
             have a narrower distribution of the momentum flow inside the
             jet area than <i>b</i>-quark jets.},
   Doi = {10.1140/epjc/s10052-013-2676-3},
   Key = {fds307642}
}

@article{fds356584,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
             Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
             NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
             J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP},
   Title = {Measurement of jet-substructure observables in top quark, W
             boson and light jet production in proton-proton collisions
             at √s = 13 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {8},
   Year = {2019},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2019)033},
   Abstract = {A measurement of jet substructure observables is presented
             using data collected in 2016 by the ATLAS experiment at the
             LHC with proton-proton collisions at s = 13 TeV.
             Large-radius jets groomed with the trimming and soft-drop
             algorithms are studied. Dedicated event selections are used
             to study jets produced by light quarks or gluons, and
             hadronically decaying top quarks and W bosons. The
             observables measured are sensitive to substructure, and
             therefore are typically used for tagging large-radius jets
             from boosted massive particles. These include the energy
             correlation functions and the N-subjettiness variables. The
             number of subjets and the Les Houches angularity are also
             considered. The distributions of the substructure variables,
             corrected for detector effects, are compared to the
             predictions of various Monte Carlo event generators. They
             are also compared between the large-radius jets originating
             from light quarks or gluons, and hadronically decaying top
             quarks and W bosons. [Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP08(2019)033},
   Key = {fds356584}
}

@article{fds356556,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
             L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
             JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA},
   Title = {Measurement of KS0 and Λ production in tt¯ dileptonic
             events in pp collisions at √s= 7 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {12},
   Year = {2019},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7512-y},
   Abstract = {Measurements of KS0 and Λ production in tt¯ final states
             have been performed. They are based on a data sample with
             integrated luminosity of 4.6 fb - 1 from proton–proton
             collisions at a centre-of-mass energy of 7 TeV, collected in
             2011 with the ATLAS detector at the Large Hadron Collider.
             Neutral strange particles are separated into three classes,
             depending on whether they are contained in a jet, with or
             without a b-tag, or not associated with a selected jet. The
             aim is to look for differences in their main kinematic
             distributions. A comparison of data with several Monte Carlo
             simulations using different hadronisation and fragmentation
             schemes, colour reconnection models and different tunes for
             the underlying event has been made. The production of
             neutral strange particles in tt¯ dileptonic events is found
             to be well described by current Monte Carlo models for KS0
             and Λ production within jets, but not for those produced
             outside jets.},
   Doi = {10.1140/epjc/s10052-019-7512-y},
   Key = {fds356556}
}

@article{fds348985,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
             C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
             AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
             R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
             JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M},
   Title = {Measurement of lepton differential distributions and the top
             quark mass in t t ¯ production in pp collisions at s
             = 8  TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {11},
   Pages = {804},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5349-9},
   Abstract = {This paper presents single lepton and dilepton kinematic
             distributions measured in dileptonic t t ¯ events produced
             in 20.2 fb - 1 of s = 8  TeV <i>pp</i> collisions recorded
             by the ATLAS experiment at the LHC. Both absolute and
             normalised differential cross-sections are measured, using
             events with an opposite-charge e μ pair and one or two
             <i>b</i>-tagged jets. The cross-sections are measured in a
             fiducial region corresponding to the detector acceptance for
             leptons, and are compared to the predictions from a variety
             of Monte Carlo event generators, as well as fixed-order QCD
             calculations, exploring the sensitivity of the
             cross-sections to the gluon parton distribution function.
             Some of the distributions are also sensitive to the top
             quark pole mass; a combined fit of NLO fixed-order
             predictions to all the measured distributions yields a top
             quark mass value of m t pole = 173.2 ± 0.9 ± 0.8 ± 1.2
              GeV, where the three uncertainties arise from data
             statistics, experimental systematics, and theoretical
             sources.},
   Doi = {10.1140/epjc/s10052-017-5349-9},
   Key = {fds348985}
}

@article{fds355784,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R},
   Title = {Measurement of light-by-light scattering and search for
             axion-like particles with 2.2 nb−1 of Pb+Pb
             data with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {3},
   Year = {2021},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2021)243},
   Abstract = {This paper describes a measurement of light-by-light
             scattering based on Pb+Pb collision data recorded by the
             ATLAS experiment during Run 2 of the LHC. The study uses 2.2
             nb−1 of integrated luminosity collected in 2015 and 2018
             at sNN = 5.02 TeV. Light-by-light scattering candidates are
             selected in events with two photons produced exclusively,
             each with transverse energy ETγ> 2.5 GeV, pseudorapidity
             |ηγ| < 2.37, diphoton invariant mass mγγ> 5 GeV, and
             with small diphoton transverse momentum and diphoton
             acoplanarity. The integrated and differential fiducial cross
             sections are measured and compared with theoretical
             predictions. The diphoton invariant mass distribution is
             used to set limits on the production of axion-like
             particles. This result provides the most stringent limits to
             date on axion-like particle production for masses in the
             range 6–100 GeV. Cross sections above 2 to 70 nb are
             excluded at the 95% CL in that mass interval. [Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP03(2021)243},
   Key = {fds355784}
}

@article{fds356696,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Measurement of long-range multiparticle azimuthal
             correlations with the subevent cumulant method in pp and p
             +Pb collisions with the ATLAS detector at the CERN Large
             Hadron Collider},
   Journal = {Physical Review C},
   Volume = {97},
   Number = {2},
   Year = {2018},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevC.97.024904},
   Abstract = {A detailed study of multiparticle azimuthal correlations is
             presented using pp data at s=5.02 and 13 TeV, and p+Pb data
             at sNN=5.02 TeV, recorded with the ATLAS detector at the
             CERN Large Hadron Collider. The azimuthal correlations are
             probed using four-particle cumulants cn{4} and flow
             coefficients vn{4}=(-cn{4})1/4 for n=2 and 3, with the goal
             of extracting long-range multiparticle azimuthal correlation
             signals and suppressing the short-range correlations. The
             values of cn{4} are obtained as a function of the average
             number of charged particles per event, Nch, using the
             recently proposed two-subevent and three-subevent cumulant
             methods, and compared with results obtained with the
             standard cumulant method. The standard method is found to be
             strongly biased by short-range correlations, which originate
             mostly from jets with a positive contribution to cn{4}. The
             three-subevent method, on the other hand, is found to be
             least sensitive to short-range correlations. The
             three-subevent method gives a negative c2{4}, and therefore
             a well-defined v2{4}, nearly independent of Nch, which
             implies that the long-range multiparticle azimuthal
             correlations persist to events with low multiplicity.
             Furthermore, v2{4} is found to be smaller than the v2{2}
             measured using the two-particle correlation method, as
             expected for long-range collective behavior. Finally, the
             measured values of v2{4} and v2{2} are used to estimate the
             number of sources relevant for the initial eccentricity in
             the collision geometry. The results based on the subevent
             cumulant technique provide direct evidence, in small
             collision systems, for a long-range collectivity involving
             many particles distributed across a broad rapidity
             interval.},
   Doi = {10.1103/PhysRevC.97.024904},
   Key = {fds356696}
}

@article{fds310353,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurement of long-range pseudorapidity correlations and
             azimuthal harmonics in √sNN =5.02 TeV
             proton-lead collisions with the ATLAS detector},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {90},
   Number = {4},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevC.90.044906},
   Abstract = {Measurements of two-particle correlation functions and the
             first five azimuthal harmonics, v1 to v5, are presented,
             using 28 nb-1 of p+Pb collisions at a nucleon-nucleon
             center-of-mass energy of √sNN=5.02 TeV measured with the
             ATLAS detector at the LHC. Significant long-range
             "ridgelike" correlations are observed for pairs with small
             (|Δϕ|<π/3) and back-to-back pairs (|Δφ|>2π/3) over the
             transverse momentum range 0.4<pT<12 GeV and in different
             intervals of event activity. The event activity is defined
             by either the number of reconstructed tracks or the total
             transverse energy on the Pb-fragmentation side. The
             azimuthal structure of such long-range correlations is
             Fourier decomposed to obtain the harmonics νn as a function
             of pT and event activity. The extracted νn values for n=2
             to 5 decrease with n. The ν2 and ν3 values are found to be
             positive in the measured pT range. The ν1 is also measured
             as a function of pT and is observed to change sign around
             pT≈1.5-2.0 GeV and then increase to about 0.1 for pT>4
             GeV. The ν2 (pT), ν3 (pT), and ν4 (pT) are compared to
             the νn coefficients in Pb+Pb collisions at √sNN=2.76 TeV
             with similar event multiplicities. Reasonable agreement is
             observed after accounting for the difference in the average
             pT of particles produced in the two collision
             systems.},
   Doi = {10.1103/PhysRevC.90.044906},
   Key = {fds310353}
}

@article{fds356549,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arling,
             JH},
   Title = {Measurement of long-range two-particle azimuthal
             correlations in Z-boson tagged pp collisions at √s=8 and
             13 TeV},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {1},
   Year = {2020},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-7606-6},
   Abstract = {Results are presented from the measurement by ATLAS of
             long-range (| Δ η| > 2) dihadron angular correlations in
             s=8 and 13 TeV pp collisions containing a Z boson. The
             analysis is performed using 19.4 fb - 1 of s=8 TeV data
             recorded during Run 1 of the LHC and 36.1 fb - 1 of
             s=13 TeV data recorded during Run 2. Two-particle
             correlation functions are measured as a function of relative
             azimuthal angle over the relative pseudorapidity range 2 < |
             Δ η| < 5 for different intervals of charged-particle
             multiplicity and transverse momentum. The measurements are
             corrected for the presence of background charged particles
             generated by collisions that occur during one passage of two
             colliding proton bunches in the LHC. Contributions to the
             two-particle correlation functions from hard processes are
             removed using a template-fitting procedure. Sinusoidal
             modulation in the correlation functions is observed and
             quantified by the second Fourier coefficient of the
             correlation function, v2 , 2, which in turn is used to
             obtain the single-particle anisotropy coefficient v2. The v2
             values in the Z-tagged events, integrated over 0.5 < pT< 5
             GeV, are found to be independent of multiplicity and s, and
             consistent within uncertainties with previous measurements
             in inclusive pp collisions. As a function of
             charged-particle pT, the Z-tagged and inclusive v2 values
             are consistent within uncertainties for pT< 3
             GeV.},
   Doi = {10.1140/epjc/s10052-020-7606-6},
   Key = {fds356549}
}

@article{fds347469,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
             C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
             AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
             O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
             R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
             JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M},
   Title = {Measurement of longitudinal flow decorrelations in Pb+Pb
             collisions at s NN = 2.76 and 5.02 TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {2},
   Pages = {142},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-5605-7},
   Abstract = {Measurements of longitudinal flow correlations are presented
             for charged particles in the pseudorapidity range | η | <
             2.4 using 7 and 470 μ b - 1 of Pb+Pb collisions at s NN =
             2.76 and 5.02 TeV, respectively, recorded by the ATLAS
             detector at the LHC. It is found that the correlation
             between the harmonic flow coefficients v n measured in two
             separated η intervals does not factorise into the product
             of single-particle coefficients, and this breaking of
             factorisation, or flow decorrelation, increases linearly
             with the η separation between the intervals. The flow
             decorrelation is stronger at 2.76 TeV than at 5.02 TeV.
             Higher-order moments of the correlations are also measured,
             and the corresponding linear coefficients for the k th
             -moment of the v n are found to be proportional to <i>k</i>
             for v 3 , but not for v 2 . The decorrelation effect is
             separated into contributions from the magnitude of v n and
             the event-plane orientation, each as a function of η .
             These two contributions are found to be comparable. The
             longitudinal flow correlations are also measured between v n
             of different order in <i>n</i>. The decorrelations of v 2
             and v 3 are found to be independent of each other, while the
             decorrelations of v 4 and v 5 are found to be driven by the
             nonlinear contribution from v 2 2 and v 2 v 3 ,
             respectively.},
   Doi = {10.1140/epjc/s10052-018-5605-7},
   Key = {fds347469}
}

@article{fds308109,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of mass and width of the excited charmed meson
             states D10 and D2*0},
   Journal = {Phys. Rev.},
   Volume = {D73},
   Number = {5},
   Pages = {051104},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.051104},
   Abstract = {We report on precision measurements of the masses and widths
             of the narrow, orbitally excited states D0_1 and D*0_2 using
             the CDF II detector at the Fermilab Tevatron. Both states
             (collectively called D**) are reconstructed in the decay
             channel D** --> D*+ pi+-. The D*0_s is also reconstructed in
             the D** --> D+ pi+- channel. Using a dataset with an
             integrated luminosity of 210 pb-1, the measured masses and
             widths for the D0_1 are 2421.7 +/- 0.7 +/- 0.6 MeV/c2 and
             20.0 +/- 1.7 +/- 1.3 MeV/c2 respectively, while for the
             D*0_2 they are 2463.3 +/- 0.6 +/- 0.8 MeV/c2 and 49.2 +/-
             2.3 +/- 1.2 MeV/c2. These values are currently the single
             best measurements available.},
   Doi = {10.1103/PhysRevD.73.051104},
   Key = {fds308109}
}

@article{fds325779,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Measurement of multi-jet cross sections in proton–proton
             collisions at a 7 TeV center-of-mass energy},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {11},
   Pages = {1-27},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1763-6},
   Abstract = {Inclusive multi-jet production is studied in proton–proton
             collisions at a center-of-mass energy of 7 TeV, using the
             ATLAS detector. The data sample corresponds to an integrated
             luminosity of 2.4 pb-1. Results on multi-jet cross sections
             are presented and compared to both leading-order plus
             parton-shower Monte Carlo predictions and to
             next-to-leading-order QCD calculations.},
   Doi = {10.1140/epjc/s10052-011-1763-6},
   Key = {fds325779}
}

@article{fds347506,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Aleksa,
             M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Santos,
             SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic,
             M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Billoud, TRV and Bilokon, H and Bindi, M and Bingul,
             A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard,
             DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair,
             RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin,
             DL and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock,
             I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
             MK and Bulekov, O and Bullock, D and Burch, TJ and Burckhart, H and Burdin,
             S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke,
             S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán,
             SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura,
             P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone,
             RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino,
             G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn,
             R and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan,
             SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
             YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca,
             D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A},
   Title = {Measurement of multi-particle azimuthal correlations in pp,
             p + Pb and low-multiplicity Pb + Pb collisions with the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {6},
   Pages = {428},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4988-1},
   Abstract = {Multi-particle cumulants and corresponding Fourier harmonics
             are measured for azimuthal angle distributions of charged
             particles in [Formula: see text] collisions at [Formula: see
             text] = 5.02 and 13 TeV and in [Formula: see text] + Pb
             collisions at [Formula: see text] = 5.02 TeV, and compared
             to the results obtained for low-multiplicity [Formula: see
             text] collisions at [Formula: see text] = 2.76 TeV. These
             measurements aim to assess the collective nature of particle
             production. The measurements of multi-particle cumulants
             confirm the evidence for collective phenomena in [Formula:
             see text] + Pb and low-multiplicity [Formula: see text]
             collisions. On the other hand, the [Formula: see text]
             results for four-particle cumulants do not demonstrate
             collective behaviour, indicating that they may be biased by
             contributions from non-flow correlations. A comparison of
             multi-particle cumulants and derived Fourier harmonics
             across different collision systems is presented as a
             function of the charged-particle multiplicity. For a given
             multiplicity, the measured Fourier harmonics are largest in
             [Formula: see text], smaller in [Formula: see text] + Pb
             and smallest in [Formula: see text] collisions. The
             [Formula: see text] results show no dependence on the
             collision energy, nor on the multiplicity.},
   Doi = {10.1140/epjc/s10052-017-4988-1},
   Key = {fds347506}
}

@article{fds372394,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
             L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
             JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
             JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
             VA},
   Title = {Measurement of muon pairs produced via γγ scattering in
             nonultraperipheral Pb + Pb collisions at √sNN = 5.02 TeV
             with the ATLAS detector},
   Journal = {Physical Review C},
   Volume = {107},
   Number = {5},
   Year = {2023},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevC.107.054907},
   Abstract = {Results of a measurement of dimuon photoproduction in
             nonultraperipheral Pb + Pb collisions at √sNN = 5.02 TeV
             are presented. Themeasurement uses ATLAS data from the 2015
             and 2018 Pb + Pb data-taking periods at the LHC with an
             integrated luminosity of 1.94 nb.1. The γγ → μ+ μ-
             pairs are identified via selections on pair momentum
             asymmetry and acoplanarity. Differential cross sections for
             dimuon production are measured in different centrality,
             average muon momentum, and pair rapidity intervals as
             functions of acoplanarity and k⊥, the transverse momentum
             kick of one muon relative to the other. Measurements are
             also made as a function of the rapidity separation of the
             muons and the angle of the muon pair relative to the
             second-order event plane to test whether magnetic fields
             generated in the quark-gluon plasma affect the measured
             muons. A prior observation of a centrality-dependent
             broadening of the acoplanarity distribution is confirmed.
             Furthermore, the improved precision of the measurement
             reveals a depletion in the number of pairs having small
             acoplanarity or k⊥ values in more central collisions. The
             acoplanarity distributions in a given centrality interval
             are observed to vary with the mean pT of the muons in the
             pair, but the k⊥ distributions do not. Comparisons with
             recent theoretical predictions are made. The predicted
             trends associated with effects of magnetic fields on the
             dimuons are not observed.},
   Doi = {10.1103/PhysRevC.107.054907},
   Key = {fds372394}
}

@booklet{Adams95c,
   Author = {Adams, MR and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Breidung, H and Busza, W and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dhawan, SK and Dietrich, FS and Dougherty,
             W and Dreyer, T and Eckardt, V and Ecker, U and Erdmann, M and Faller, F and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen, KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Hughes, VW and Jackson, HE and Jancso, G and Jansen, DM and Jin, Z and Kaufman, S and Kennedy, RD and Kinney, ER and Kirk, T and Kobrak, HG and Kotwal, AV and Kunori, S and Lancaster, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin, JG and Nickerson, RB and O'Day, S and Olkiewicz, K and Osborne, L and Otten,
             R},
   Title = {Measurement of nuclear transparencies from exclusive rho 0
             meson production in muon-nucleus scattering at 470
             GeV.},
   Journal = {Physical review letters},
   Volume = {74},
   Number = {9},
   Pages = {1525-1529},
   Year = {1995},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.74.1525},
   Doi = {10.1103/physrevlett.74.1525},
   Key = {Adams95c}
}

@article{fds308156,
   Author = {Acosta, D and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
             J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura, P and Campanelli, M and Campbell, M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri,
             A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
             JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
             J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
             N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, J and Frisch,
             H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti,
             P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
             M and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
             D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
             KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
             PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
             BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu,
             T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic,
             P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin,
             A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
             C and Nicollerat, AS and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa,
             T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patricck, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pitts, KT and Plager, C and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio,
             S and Ratnikov, F and Ray, H and Reichold, A and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna,
             G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar,
             S and Sato, K and Savard, P and Savoy-Navarro, A and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shochet,
             M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba, A and Slaughter, AJ and Sliwa, K and Smirnov, D and Smith, JR and Snider,
             FD},
   Title = {Measurement of partial widths and search for direct CP
             violation in D 0 meson decays to
             K-K+ and π -π+},
   Journal = {Physical Review Letters},
   Volume = {94},
   Number = {12},
   Pages = {122001},
   Year = {2005},
   ISSN = {0031-9007},
   url = {http://www.ncbi.nlm.nih.gov/pubmed/15903906},
   Abstract = {We present a measurement of relative partial widths and
             decay rate CP asymmetries in K- K+ and π-π+ decays of D0
             mesons produced in pp̄ collisions at,√s = 1.96 TeV. We
             use a sample of 2 × 105 D*+ →D0π+ (and charge conjugate)
             decays with the D0 decaying to K-π+, K-K +, and π-π+,
             corresponding to 123 pb -1 of data collected by the Collider
             Detector at Fermilab II experiment at the Fermilab Tevatron
             collider. No significant direct CP violation is observed. We
             measure γ(D0→ K- K +)/γ(D0-→K-π+) = 0.0992 ±0.0992
             ±0.0012, γ(D0→K -π+)/γ(D0→K -π+) = 0.03594 ±
             0.00054 ±0.00040, A CP(K- K+) = (2.0 ±1.2 ±0.6)%, and
             ACP(π-π+) = (1.0 ±1.3 ±0.6)%, where, in all cases, the
             first uncertainty is statistical and the second is
             systematic. © 2005 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.94.122001},
   Key = {fds308156}
}

@article{fds307993,
   Author = {Aaltonen, T and others},
   Title = {Measurement of particle production and inclusive
             differential cross sections in pp̅ collisions at sqrt[s]
             =1.96 TeV},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {11},
   Pages = {112005},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.112005},
   Abstract = {We report a set of measurements of particle production in
             inelastic pp̅ collisions collected with a minimum-bias
             trigger at the Tevatron Collider with the CDF II experiment.
             The inclusive charged particle transverse momentum
             differential cross section is measured, with improved
             precision, over a range about ten times wider than in
             previous measurements. The former modeling of the spectrum
             appears to be incompatible with the high particle momenta
             observed. The dependence of the charged particle transverse
             momentum on the event particle multiplicity is analyzed to
             study the various components of hadron interactions. This is
             one of the observable variables most poorly reproduced by
             the available Monte Carlo generators. A first measurement of
             the event transverse energy sum differential cross section
             is also reported. A comparison with a pythia prediction at
             the hadron level is performed. The inclusive
             charged-particle differential production cross section is
             fairly well reproduced only in the transverse momentum range
             available from previous measurements. At higher momentum the
             agreement is poor. The transverse energy sum is poorly
             reproduced over the whole spectrum. The dependence of the
             charged particle transverse momentum on the particle
             multiplicity needs the introduction of more sophisticated
             particle production mechanisms, such as multiple parton
             interactions, in order to be better explained.},
   Doi = {10.1103/PhysRevD.79.112005},
   Key = {fds307993}
}

@article{fds356624,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Measurement of photon–jet transverse momentum correlations
             in 5.02 TeV Pb + Pb and pp collisions with
             ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {789},
   Pages = {167-190},
   Year = {2019},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.12.023},
   Abstract = {Jets created in association with a photon can be used as a
             calibrated probe to study energy loss in the medium created
             in nuclear collisions. Measurements of the transverse
             momentum balance between isolated photons and inclusive jets
             are presented using integrated luminosities of 0.49 nb−1
             of Pb + Pb collision data at sNN=5.02 TeV and 25 pb−1 of
             pp collision data at s=5.02 TeV recorded with the ATLAS
             detector at the LHC. Photons with transverse momentum
             63.1<pTγ<200 GeV and |ηγ|<2.37 are paired with all jets
             in the event that have pTjet>31.6 GeV and pseudorapidity
             |ηjet|<2.8. The transverse momentum balance given by the
             jet-to-photon pT ratio, xJγ, is measured for pairs with
             azimuthal opening angle Δϕ>7π/8. Distributions of the
             per-photon jet yield as a function of xJγ,
             (1/Nγ)(dN/dxJγ), are corrected for detector effects via a
             two-dimensional unfolding procedure and reported at the
             particle level. In pp collisions, the distributions are well
             described by Monte Carlo event generators. In Pb + Pb
             collisions, the xJγ distribution is modified from that
             observed in pp collisions with increasing centrality,
             consistent with the picture of parton energy loss in the hot
             nuclear medium. The data are compared with a suite of
             energy-loss models and calculations.},
   Doi = {10.1016/j.physletb.2018.12.023},
   Key = {fds356624}
}

@article{fds307829,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
             M and de Barbaro, P and De Cecco and S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
             G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
             JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
             K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
             M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker,
             A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee,
             E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rosner, JL and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel,
             S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and Denis,
             RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
             J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel,
             M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester,
             WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang,
             YC},
   Title = {Measurement of polarization and search for CP violation in
             B(s)0→φφ decays.},
   Journal = {Physical review letters},
   Volume = {107},
   Number = {26},
   Pages = {261802},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.107.261802},
   Abstract = {We present the first measurement of polarization and
             CP-violating asymmetries in a B(s)(0) decay into two light
             vector mesons, B(s)(0)→φφ, and an improved determination
             of its branching ratio using 295 decays reconstructed in a
             data sample corresponding to 2.9 fb(-1) of integrated
             luminosity collected by the CDF experiment at the Fermilab
             Tevatron collider. The fraction of longitudinal polarization
             is determined to be f(L)=0.348±0.041(stat)±0.021(syst),
             and the branching ratio B(B(s)(0)→φφ)=[2.32±0.18(stat)±0.82(syst)]×10(-5).
             Asymmetries of decay angle distributions sensitive to CP
             violation are measured to be A(u)=-0.007±0.064(stat)±0.018(syst)
             and A(v)=-0.120±0.064(stat)±0.016(syst).},
   Doi = {10.1103/physrevlett.107.261802},
   Key = {fds307829}
}

@article{fds308167,
   Author = {Collaboration, DAEACDFII},
   Title = {Measurement of Prompt Charm Meson Production Cross Sections
             in pp-bar Collisions at sqrt[s]=1.96 TeV},
   Journal = {Physical Review Letters},
   Volume = {91},
   Number = {24},
   Pages = {241804},
   Year = {2003},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.91.241804},
   Abstract = {We report on measurements of differential cross sections d
             sigma /dpT for prompt charm meson production in pp-bar
             collisions at sqrt[s]=1.96 TeV using 5.8±0.3 pb-1 of data
             from the CDF II detector at the Fermilab Tevatron. The data
             are collected with a new trigger that is sensitive to the
             long lifetime of hadrons containing heavy flavor. The charm
             meson cross sections are measured in the central rapidity
             region |y| K- pi +, D*+-->D0 pi +, D+-->K- pi + pi +, D+s-->
             phi pi +, and their charge conjugates. The measured cross
             sections are compared to theoretical calculations.},
   Doi = {10.1103/physrevlett.91.241804},
   Key = {fds308167}
}

@article{fds356576,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
             JF},
   Title = {Measurement of prompt photon production in
             sNN=8.16 TeV p + Pb collisions with
             ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {796},
   Pages = {230-252},
   Year = {2019},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.07.031},
   Abstract = {The inclusive production rates of isolated, prompt photons
             in p+Pb collisions at sNN=8.16 TeV are studied with the
             ATLAS detector at the Large Hadron Collider using a dataset
             with an integrated luminosity of 165 nb−1 recorded in
             2016. The cross-section and nuclear modification factor RpPb
             are measured as a function of photon transverse energy from
             20 GeV to 550 GeV and in three nucleon–nucleon
             centre-of-mass pseudorapidity regions, (−2.83,−2.02),
             (−1.84,0.91), and (1.09,1.90). The cross-section and RpPb
             values are compared with the results of a
             next-to-leading-order perturbative QCD calculation, with and
             without nuclear parton distribution function modifications,
             and with expectations based on a model of the energy loss of
             partons prior to the hard scattering. The data disfavour a
             large amount of energy loss and provide new constraints on
             the parton densities in nuclei.},
   Doi = {10.1016/j.physletb.2019.07.031},
   Key = {fds356576}
}

@article{fds347470,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
             De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A},
   Title = {Measurement of quarkonium production in proton-lead and
             proton-proton collisions at 5.02 TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {3},
   Pages = {171},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-5624-4},
   Abstract = {The modification of the production of J / ψ , ψ ( 2 S ) ,
             and Υ ( n S ) ( n = 1 , 2 , 3 ) in <i>p</i>+Pb collisions
             with respect to their production in <i>pp</i> collisions has
             been studied. The <i>p</i>+Pb and <i>pp</i> datasets used in
             this paper correspond to integrated luminosities of 28 nb -
             1 and 25 pb - 1 respectively, collected in 2013 and 2015 by
             the ATLAS detector at the LHC, both at a centre-of-mass
             energy per nucleon pair of 5.02 TeV. The quarkonium states
             are reconstructed in the dimuon decay channel. The yields of
             J / ψ and ψ ( 2 S ) are separated into prompt and
             non-prompt sources. The measured quarkonium differential
             cross sections are presented as a function of rapidity and
             transverse momentum, as is the nuclear modification factor,
             R p Pb for J / ψ and Υ ( n S ) . No significant
             modification of the J / ψ production is observed while Υ (
             n S ) production is found to be suppressed at low transverse
             momentum in <i>p</i>+Pb collisions relative to <i>pp</i>
             collisions. The production of excited charmonium and
             bottomonium states is found to be suppressed relative to
             that of the ground states in central <i>p</i>+Pb
             collisions.},
   Doi = {10.1140/epjc/s10052-018-5624-4},
   Key = {fds347470}
}

@article{fds307599,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Measurement of R=B(t→Wb)/B(t→Wq) in top-quark-pair
             decays using lepton+jets events and the full CDF run II
             dataset},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.111101},
   Abstract = {We present a measurement of the ratio of the top-quark
             branching fractions R=B(t→Wb)/B(t→Wq), where q
             represents quarks of type b, s, or d, in the final state
             with a lepton and hadronic jets. The measurement uses
             √s=1.96 TeV proton-antiproton collision data from 8.7 fb-1
             of integrated luminosity collected with the Collider
             Detector at Fermilab during Run II of the Tevatron. We
             simultaneously measure R=0.94±0.09 (stat+syst) and the tt̄
             production cross section σtt̄=7. 5±1.0 (stat+syst) pb.
             The magnitude of the Cabibbo-Kobayashi-Maskawa matrix
             element, |Vtb|=0.97±0.05 (stat+syst) is extracted assuming
             three generations of quarks, and a lower limit of |V
             tb|>0.89 at 95% credibility level is set. © 2013 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.87.111101},
   Key = {fds307599}
}

@article{fds307957,
   Author = {Aaltonen, T and others},
   Title = {Measurement of Resonance Parameters of Orbitally Excited
             Narrow B[sup 0] Mesons},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {10},
   Pages = {102003},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.102003},
   Abstract = {We report a measurement of resonance parameters of the
             orbitally excited (L=1) narrow B0 mesons in decays to
             B;{(*)+}pi;{-} using 1.7 fb;{-1} of data collected by the
             CDF II detector at the Fermilab Tevatron. The mass and width
             of the B_{2};{*0} state are measured to be
             m(B_{2};{*0})=5740.2_{-1.8};{+1.7}(stat)-0.8+0.9(syst)
             MeV/c;{2} and Gamma(B_{2};{*0})=22.7_{-3.2};{+3.8}(stat)-10.2+3.2(syst)
             MeV/c;{2}. The mass difference between the B_{2};{*0} and
             B10 states is measured to be 14.9_{-2.5};{+2.2}(stat)-1.4+1.2(syst)
             MeV/c;{2}, resulting in a B10 mass of 5725.3_{-2.2};{+1.6}(stat)-1.5+1.4(syst)
             MeV/c;{2}. This is currently the most precise measurement of
             the masses of these states and the first measurement of the
             B_{2};{*0} width.},
   Doi = {10.1103/physrevlett.102.102003},
   Key = {fds307957}
}

@article{fds308080,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, J-F and Arisawa, T and Artikov, A and Ashmanskas, W and Attal,
             A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Casarsa, M and Castro,
             A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Cyr,
             D and DaRonco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and de Barbaro, P and De Cecco and S and Deisher, A and De
             Lentdecker, G and Dell'Orso, M and Delli Paoli and F and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni,
             GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and DiTuro, P and Dörr,
             C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes,
             D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Gimmell,
             JL and Ginsburg, C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Guimaraes da
             Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
             RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
             A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
             S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Le, Y and LeCompte, T and Lee, J and Lee,
             YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister,
             A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
             M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean,
             R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Movilla
             Fernandez, P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nagano, A and Naganoma, J and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse,
             E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ranjan,
             N and Rappoccio, S and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
             R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Sjolin, J},
   Title = {Measurement of sigma Lambda b0/sigma B0 x B(Lambda
             b0-->Lambda c+pi-)/B(B0-->D+pi-) in pp collisions at square
             root s=1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {98},
   Number = {12},
   Pages = {122002},
   Year = {2007},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.98.122002},
   Abstract = {We present the first observation of the baryon decay Lambda
             b0-->Lambda c+pi- followed by Lambda c+-->pK-pi+ in 106 pb-1
             pp collisions at square root s=1.96 TeV in the CDF
             experiment. In order to reduce systematic error, the
             measured rate for Lambda b0 decay is normalized to the
             kinematically similar meson decay B0-->D+pi- followed by
             D+-->pi+K-pi+. We report the ratio of production cross
             sections (sigma) times the ratio of branching fractions (B)
             for the momentum region integrated above pT>6 GeV/c and
             pseudorapidity range |eta|<1.3: sigma(pp-->Lambda
             b0X)/sigma(pp-->B0X)xB(Lambda b0-->Lambda
             c+pi-)/B(B0-->D+pi-)=0.82+/-0.08(stat)+/-0.11(syst)+/-0.22[B(Lambda
             c+-->pK-pi+)].},
   Doi = {10.1103/physrevlett.98.122002},
   Key = {fds308080}
}

@article{fds321122,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Erbacher, R and Errede, S and Esham,
             B},
   Title = {Measurement of sin2 θefflept
             using e+e- pairs from γ/Z bosons produced in
             pp collisions at a center-of-momentum energy of 1.96
             TeV},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.112016},
   Abstract = {At the Fermilab Tevatron proton-antiproton (pp) collider,
             Drell-Yan lepton pairs are produced in the process
             pp→e+e-+X through an intermediate γ∗/Z boson. The
             forward-backward asymmetry in the polar-angle distribution
             of the e- as a function of the e+e - pair mass is used to
             obtain sin2θefflept, the effective leptonic determination
             of the electroweak-mixing parameter sin2θW. The measurement
             sample, recorded by the Collider Detector at Fermilab (CDF),
             corresponds to 9.4 fb-1 of integrated luminosity from pp
             collisions at a center-of-momentum energy of 1.96 TeV, and
             is the full CDF Run II data set. The value of sin2θefflept
             is found to be 0.23248±0.00053. The combination with the
             previous CDF measurement based on μ+μ- pairs yields
             sin2θefflept=0.23221±0.00046. This result, when
             interpreted within the specified context of the standard
             model assuming sin2θW=1-MW2/MZ2 and that the W- and Z-boson
             masses are on-shell, yields sin2θW=0.22400±0.00045, or
             equivalently a W-boson mass of 80.328±0.024
             GeV/c2.},
   Doi = {10.1103/PhysRevD.93.112016},
   Key = {fds321122}
}

@article{fds358461,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Pozo, JAA and Bella, LA and Arabidze, G},
   Title = {Measurement of single top-quark production in association
             with a W boson in the single-lepton channel at √s=8TeV
             with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {8},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09371-7},
   Abstract = {The production cross-section of a top quark in association
             with a W boson is measured using proton–proton collisions
             at s=8TeV. The dataset corresponds to an integrated
             luminosity of 20.2fb-1, and was collected in 2012 by the
             ATLAS detector at the Large Hadron Collider at CERN. The
             analysis is performed in the single-lepton channel. Events
             are selected by requiring one isolated lepton (electron or
             muon) and at least three jets. A neural network is trained
             to separate the tW signal from the dominant tt¯ background.
             The cross-section is extracted from a binned profile
             maximum-likelihood fit to a two-dimensional discriminant
             built from the neural-network output and the invariant mass
             of the hadronically decaying W boson. The measured
             cross-section is σtW=26±7pb, in good agreement with the
             Standard Model expectation.},
   Doi = {10.1140/epjc/s10052-021-09371-7},
   Key = {fds358461}
}

@article{fds349430,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH},
   Title = {Measurement of soft-drop jet observables in pp collisions
             with the ATLAS detector at s =13 TeV},
   Journal = {Physical Review D},
   Volume = {101},
   Number = {5},
   Year = {2020},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.101.052007},
   Abstract = {Jet substructure quantities are measured using jets groomed
             with the soft-drop grooming procedure in dijet events from
             32.9 fb-1 of pp collisions collected with the ATLAS detector
             at s=13 TeV. These observables are sensitive to a wide range
             of QCD phenomena. Some observables, such as the jet mass and
             opening angle between the two subjets which pass the
             soft-drop condition, can be described by a high-order
             (resummed) series in the strong coupling constant αS. Other
             observables, such as the momentum sharing between the two
             subjets, are nearly independent of αS. These observables
             can be constructed using all interacting particles or using
             only charged particles reconstructed in the inner tracking
             detectors. Track-based versions of these observables are not
             collinear safe, but are measured more precisely, and
             universal nonperturbative functions can absorb the collinear
             singularities. The unfolded data are directly compared with
             QCD calculations and hadron-level Monte Carlo simulations.
             The measurements are performed in different pseudorapidity
             regions, which are then used to extract quark and gluon jet
             shapes using the predicted quark and gluon fractions in each
             region. All of the parton shower and analytical calculations
             provide an excellent description of the data in most regions
             of phase space.},
   Doi = {10.1103/PhysRevD.101.052007},
   Key = {fds349430}
}

@article{fds310291,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Azuma, Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli,
             F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak,
             L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi,
             M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov,
             AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron,
             J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
             AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T},
   Title = {Measurement of spin correlation in top-antitop quark events
             and search for top squark pair production in pp collisions
             at √s=8  TeV using the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {14},
   Pages = {142001},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.114.142001},
   Abstract = {A measurement of spin correlation in tt[over ¯] production
             is presented using data collected with the ATLAS detector at
             the Large Hadron Collider in proton-proton collisions at a
             center-of-mass energy of 8 TeV, corresponding to an
             integrated luminosity of 20.3  fb^{-1}. The correlation
             between the top and antitop quark spins is extracted from
             dilepton tt[over ¯] events by using the difference in the
             azimuthal angle between the two charged leptons in the
             laboratory frame. In the helicity basis the measured degree
             of correlation corresponds to A_{helicity}=0.38±0.04, in
             agreement with the standard model prediction. A search is
             performed for pair production of top squarks with masses
             close to the top quark mass decaying to predominantly
             right-handed top quarks and a light neutralino, the lightest
             supersymmetric particle. Top squarks with masses between the
             top quark mass and 191 GeV are excluded at the 95%
             confidence level.},
   Doi = {10.1103/physrevlett.114.142001},
   Key = {fds310291}
}

@article{fds372391,
   Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk
             Cakir, I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin,
             T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben,
             M and Bouquet, R and Marchiori, G and Bhopatkar, VS and Chekanov, S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
             Gemmeren, P and Wang, R and Zhang, J and Berlendis, S and Cheu, E and Cui,
             Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Unal, M and Webb, AF and Huseynov, N and Ahmadov, F and Agaras, MN and Bosman,
             M},
   Title = {Measurement of substructure-dependent jet suppression in
             Pb+Pb collisions at 5.02 TeV with the ATLAS
             detector},
   Journal = {Physical Review C},
   Volume = {107},
   Number = {5},
   Year = {2023},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevC.107.054909},
   Abstract = {The ATLAS detector at the Large Hadron Collider has been
             used to measure jet substructure modification and
             suppression in Pb+Pb collisions at a nucleon–nucleon
             center-of-mass energy √sNN = 5.02 TeV in comparison with
             proton–proton (pp) collisions at √s = 5.02 TeV. The
             Pb+Pb data, collected in 2018, have an integrated luminosity
             of 1.72 nb−1, while the ppdata, collected in 2017, have an
             integrated luminosity of 260 pb−1. Jets used in this
             analysis are clustered using the anti-kt algorithm with a
             radius parameter R = 0.4. The jet constituents, defined by
             both tracking and calorimeter information, are used to
             determine the angular scale rg of the first hard splitting
             inside the jet by reclustering them using the
             Cambridge–Aachen algorithm and employing the soft-drop
             grooming technique. The nuclear modification factor, RAA,
             used to characterize jet suppression in Pb+Pb collisions, is
             presented differentially in rg, jet transverse momentum, and
             in intervals of collision centrality. The RAA value is
             observed to depend significantly on jet rg. Jets produced
             with the largest measured rg are found to be twice as
             suppressed as those with the smallest rg in central Pb+Pb
             collisions. The RAA values do not exhibit a strong variation
             with jet pT in any of the rg intervals. The rg and pT
             dependence of jet RAA is qualitatively consistent with a
             picture of jet quenching arising from coherence and provides
             the most direct evidence in support of this
             approach.},
   Doi = {10.1103/PhysRevC.107.054909},
   Key = {fds372391}
}

@article{fds373907,
   Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
             M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
             PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
             Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
             V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai,
             K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos,
             R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
             PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends,
             KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron
             Moreno, DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco
             Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga,
             D and Bauce, M and Bauer, P and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli,
             M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
             L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya,
             DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel,
             O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul,
             A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman,
             M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger,
             D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruncko,
             D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
             AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
             Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson,
             BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter,
             JWS and Carter, TM and Casado, MP and Casha, AF and Caspar, M and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen,
             A and Chen, B and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark, A and Clark, PJ and Clavijo
             Columbie, JM and Clawson, SE and Clement, C and Clercx, J and Clissa, L and Coadou, Y and Cobal, M and Coccaro, A and Barrue, RFC and Coelho Lopes
             De Sa and R},
   Title = {Measurement of Suppression of Large-Radius Jets and Its
             Dependence on Substructure in Pb+Pb Collisions at
             sqrt[s_{NN}]=5.02  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {131},
   Number = {17},
   Pages = {172301},
   Year = {2023},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.131.172301},
   Abstract = {This letter presents a measurement of the nuclear
             modification factor of large-radius jets in
             sqrt[s_{NN}]=5.02  TeV Pb+Pb collisions by the ATLAS
             experiment. The measurement is performed using
             1.72  nb^{-1} and 257  pb^{-1} of Pb+Pb and pp data,
             respectively. The large-radius jets are reconstructed with
             the anti-k_{t} algorithm using a radius parameter of R=1.0,
             by reclustering anti-k_{t} R=0.2 jets, and are measured over
             the transverse momentum (p_{T}) kinematic range of
             158<p_{T}<1000  GeV and absolute pseudorapidity |y|<2.0.
             The large-radius jet constituents are further reclustered
             using the k_{t} algorithm in order to obtain the splitting
             parameters, sqrt[d_{12}] and ΔR_{12}, which characterize
             the transverse momentum scale and angular separation for the
             hardest splitting in the jet, respectively. The nuclear
             modification factor, R_{AA}, obtained by comparing the Pb+Pb
             jet yields to those in pp collisions, is measured as a
             function of jet transverse momentum (p_{T}) and sqrt[d_{12}]
             or ΔR_{12}. A significant difference in the quenching of
             large-radius jets having single subjet and those with more
             complex substructure is observed. Systematic comparison of
             jet suppression in terms of R_{AA} for different jet
             definitions is also provided. Presented results support the
             hypothesis that jets with hard internal splittings lose more
             energy through quenching and provide a new perspective for
             understanding the role of jet structure in jet
             suppression.},
   Doi = {10.1103/physrevlett.131.172301},
   Key = {fds373907}
}

@article{fds308068,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the $p \bar{p} \to t \bar{t}$ production
             cross- section and the top quark mass at $\sqrt{s}$ = 1.96-
             TeV in the all-hadronic decay mode},
   Journal = {Phys. Rev.},
   Volume = {D76},
   Number = {7},
   Pages = {072009},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.76.072009},
   Abstract = {We report the measurements of the t[overline t] production
             cross section and of the top quark mass using 1.02 fb-1 of
             p[overline p] data collected with the CDF II detector at the
             Fermilab Tevatron. We select events with six or more jets on
             which a number of kinematical requirements are imposed by
             means of a neural network algorithm. At least one of these
             jets must be identified as initiated by a b-quark candidate
             by the reconstruction of a secondary vertex. The cross
             section is measured to be sigmat[overline
             t]=8.3$\pm$1.0(stat)-1.5+2.0(syst)$\pm$0.5(lumi) pb, which
             is consistent with the standard model prediction. The top
             quark mass of 174.0$\pm$2.2(stat)$\pm$4.8(syst) GeV/c2 is
             derived from a likelihood fit incorporating reconstructed
             mass distributions representative of signal and
             background.},
   Doi = {10.1103/PhysRevD.76.072009},
   Key = {fds308068}
}

@article{fds307915,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the $t \bar{t}$ Production Cross Section in
             $p \bar{p}$ Collisions at $\sqrt{s} = 1.96$ TeV using Soft
             Electron $b$-Tagging},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {9},
   Pages = {092002},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.092002},
   Abstract = {http://arxiv.org/abs/1002.3783},
   Doi = {10.1103/PhysRevD.81.092002},
   Key = {fds307915}
}

@article{fds308095,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the $t\bar{t}$ production cross section in
             $p\bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV using missing
             $E_t$ + jets events with secondary vertex $b-
             $tagging},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {20},
   Pages = {202002},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.202002},
   Abstract = {We present a measurement of the tt-bar production cross
             section in p anti-p collisions at s**(1/2) = 1.96 TeV which
             uses events with an inclusive signature of significant
             missing transverse energy and jets. This is the first
             measurement which makes no explicit lepton identification
             requirements, so that sensitivity to W --> tau nu decays is
             maintained. Heavy flavor jets from top quark decay are
             identified with a secondary vertex tagging algorithm. From
             311 pb-1 of data collected by the Collider Detector at
             Fermilab we measure a production cross section of 5.8 +/-
             1.2(stat.)+0.9_-0.7(syst.) pb for a top quark mass of 178
             GeV/c2, in agreement with previous determinations and
             standard model predictions.},
   Doi = {10.1103/physrevlett.96.202002},
   Key = {fds308095}
}

@article{fds307879,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of the $t\overline{t}$ production cross section
             in $p\overline{p}$ collisions at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$
             using events with large missing transverse energy and
             jets},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {3},
   Pages = {032003},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.032003},
   Abstract = {In this paper we report a measurement of the tt̄ production
             cross section in pp̄ collisions at √s=1.96TeV using data
             corresponding to an integrated luminosity of 2.2fb-1
             collected with the CDF II detector at the Tevatron
             accelerator. We select events with significant missing
             transverse energy and high jet multiplicity. This
             measurement vetoes the presence of explicitly identified
             electrons and muons, thus enhancing the tau contribution of
             tt̄ decays. Signal events are discriminated from the
             background using a neural network, and heavy flavor jets are
             identified by a secondary-vertex tagging algorithm. We
             measure a tt̄ production cross section of
             7.99±0.55(stat)±0.76(syst)±0.46(lumi) pb, assuming a top
             mass mtop=172.5GeV/c2, in agreement with previous
             measurements and standard model predictions. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.84.032003},
   Key = {fds307879}
}

@article{fds307874,
   Author = {Aaltonen, and and, T and al, E},
   Title = {Measurement of the $t\overline{t}$ production cross section
             with an \textit{in~situ} calibration of $b$-jet
             identification efficiency},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {7},
   Pages = {071102},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.071102},
   Abstract = {A measurement of the top-quark pair-production cross section
             in pp̄ collisions at √s=1.96TeV using data corresponding
             to an integrated luminosity of 1.12fb-1 collected with the
             Collider Detector at Fermilab is presented. Decays of
             top-quark pairs into the final states eν+ jets and μν+
             jets are selected, and the cross section and the b-jet
             identification efficiency are determined using a new
             measurement technique which requires agreement between the
             measured cross sections with exactly one and with multiple
             identified b quarks from the top-quark decays. Assuming a
             top-quark mass of 175GeV/c2, a cross section of
             8.5±0.6(stat)±0. 7(syst)pb is measured. © 2011 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.83.071102},
   Key = {fds307874}
}

@article{fds307934,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the $WW+WZ$ production cross section using a
             matrix element technique in $lepton+jets$
             events},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {11},
   Pages = {112001},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.112001},
   Abstract = {We present a measurement of the WW+WZ production cross
             section observed in a final state consisting of an
             identified electron or muon, two jets, and missing
             transverse energy. The measurement is carried out in a data
             sample corresponding to up to 4.6fb⊃-1 of integrated
             luminosity at √s=1.96TeV collected by the CDF II detector.
             Matrix element calculations are used to separate the diboson
             signal from the large backgrounds. The WW+WZ cross section
             is measured to be 17.4±3.3pb in agreement with standard
             model predictions. A fit to the dijet invariant mass
             spectrum yields a compatible cross section measurement. ©
             2010 The American Physical Society.},
   Doi = {10.1103/PhysRevD.82.112001},
   Key = {fds307934}
}

@article{fds307909,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the $WW+WZ$ Production Cross Section Using
             the Lepton+Jets Final State at CDF II},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {10},
   Pages = {101801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.101801},
   Abstract = {http://arxiv.org/abs/0911.4449},
   Doi = {10.1103/PhysRevLett.104.101801},
   Key = {fds307909}
}

@article{fds307904,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the $W^+W^-$ Production Cross Section and
             Search for Anomalous $WW\gamma$ and $WWZ$ Couplings in $p
             \bar p$ Collisions at $\sqrt{s} = 1.96$ TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {20},
   Pages = {201801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.201801},
   Abstract = {http://arxiv.org/abs/0912.4500},
   Doi = {10.1103/PhysRevLett.104.201801},
   Key = {fds307904}
}

@article{fds307908,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the $\Lambda_b$ Lifetime in $\Lambda_b \to
             \Lambda_c^+ \pi^-$ Decays in $p\bar{p}$ Collisions at
             $\sqrt{s} = 1.96$ TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {10},
   Pages = {102002},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.102002},
   Abstract = {http://arxiv.org/abs/0912.3566},
   Doi = {10.1103/PhysRevLett.104.102002},
   Key = {fds307908}
}

@article{fds307868,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of the ${B}^{-}$ lifetime using a simulation
             free approach for trigger bias correction},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {3},
   Pages = {032008},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.032008},
   Abstract = {The collection of a large number of B-hadron decays to
             hadronic final states at the CDF II Detector is possible due
             to the presence of a trigger that selects events based on
             track impact parameters. However, the nature of the
             selection requirements of the trigger introduces a large
             bias in the observed proper-decay-time distribution. A
             lifetime measurement must correct for this bias, and the
             conventional approach has been to use a Monte Carlo
             simulation. The leading sources of systematic uncertainty in
             the conventional approach are due to differences between the
             data and the Monte Carlo simulation. In this paper, we
             present an analytic method for bias correction without using
             simulation, thereby removing any uncertainty due to the
             differences between data and simulation. This method is
             presented in the form of a measurement of the lifetime of
             the B- using the mode B-→D0π -. The B- lifetime is
             measured as τB -=1.663±0.023±0.015ps, where the first
             uncertainty is statistical and the second systematic. This
             new method results in a smaller systematic uncertainty in
             comparison to methods that use simulation to correct for the
             trigger bias. © 2011 American Physical Society.},
   Doi = {10.1103/PhysRevD.83.032008},
   Key = {fds307868}
}

@article{fds347498,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
             H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
             A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti,
             M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
             J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho,
             J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
             Alberich, L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan,
             SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont,
             AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
   Title = {Measurement of the W boson polarisation in [Formula:
             see text] events from pp collisions at [Formula: see
             text] = 8 TeV in the lepton + jets channel with
             ATLAS.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {4},
   Pages = {264},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4819-4},
   Abstract = {This paper presents a measurement of the polarisation of
             <i>W</i> bosons from [Formula: see text] decays,
             reconstructed in events with one high-[Formula: see text]
             lepton and at least four jets. Data from <i>pp</i>
             collisions at the LHC were collected at [Formula: see text]
             = 8 TeV and correspond to an integrated luminosity of
             20.2 fb[Formula: see text]. The angle [Formula: see text]
             between the <i>b</i>-quark from the top quark decay and a
             direct <i>W</i> boson decay product in the <i>W</i> boson
             rest frame is sensitive to the <i>W</i> boson polarisation.
             Two different <i>W</i> decay products are used as
             polarisation analysers: the charged lepton and the down-type
             quark for the leptonically and hadronically decaying
             <i>W</i> boson, respectively. The most precise measurement
             of the <i>W</i> boson polarisation via the distribution of
             [Formula: see text] is obtained using the leptonic analyser
             and events in which at least two of the jets are tagged as
             <i>b</i>-quark jets. The fitted fractions of longitudinal,
             left- and right-handed polarisation states are [Formula: see
             text], [Formula: see text] and [Formula: see text], and are
             the most precisely measured <i>W</i> boson polarisation
             fractions to date. Limits on anomalous couplings of the
             <i>Wtb</i> vertex are set.},
   Doi = {10.1140/epjc/s10052-017-4819-4},
   Key = {fds347498}
}

@article{fds347466,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
             M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Biebel, O and Biedermann, D and Bianco, M and Bielski,
             R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado,
             MP and Casolino, M and Casper, DW and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark,
             MR},
   Title = {Measurement of the W-boson mass in pp collisions at s
             = 7 TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {2},
   Pages = {110},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5475-4},
   Abstract = {A measurement of the mass of the <i>W</i> boson is presented
             based on proton-proton collision data recorded in 2011 at a
             centre-of-mass energy of 7 TeV with the ATLAS detector at
             the LHC, and corresponding to 4.6 fb - 1 of integrated
             luminosity. The selected data sample consists of 7.8 × 10 6
             candidates in the W → μ ν channel and 5.9 × 10 6
             candidates in the W → e ν channel. The <i>W</i>-boson
             mass is obtained from template fits to the reconstructed
             distributions of the charged lepton transverse momentum and
             of the <i>W</i> boson transverse mass in the electron and
             muon decay channels, yielding m W = 80370 ± 7 ( stat. ) ±
             11 ( exp. syst. ) ± 14 ( mod. syst. ) MeV = 80370 ± 19 MeV
             , where the first uncertainty is statistical, the second
             corresponds to the experimental systematic uncertainty, and
             the third to the physics-modelling systematic uncertainty. A
             measurement of the mass difference between the W + and W -
             bosons yields m W + - m W - = - 29 ± 28
              MeV.},
   Doi = {10.1140/epjc/s10052-017-5475-4},
   Key = {fds347466}
}

@article{fds321113,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Measurement of the angular coefficients in Z-boson events
             using electron and muon pairs from data taken at √s = 8
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2016)159},
   Abstract = {The angular distributions of Drell-Yan charged lepton pairs
             in the vicinity of the Z-boson mass peak probe the
             underlying QCD dynamics of Z-boson production. This paper
             presents a measurement of the complete set of angular
             coefficients A0−7 describing these distributions in the
             Z-boson Collins-Soper frame. The data analysed correspond to
             20.3 fb−1 of pp collisions at s=8 TeV, collected by the
             ATLAS detector at the CERN LHC. The measurements are
             compared to the most precise fixed-order calculations
             currently available (O(αs2)) and with theoretical
             predictions embedded in Monte Carlo generators. The
             measurements are precise enough to probe QCD corrections
             beyond the formal accuracy of these calculations and to
             provide discrimination between different parton-shower
             models. A significant deviation from the (O(αs2))
             predictions is observed for A0 − A2. Evidence is found for
             non-zero A5,6,7, consistent with expectations.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP08(2016)159},
   Key = {fds321113}
}

@article{fds332356,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
             JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
             R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
             D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada,
             J},
   Title = {Measurement of the angular distribution of electrons from
             [Formula Presented] decays observed in [Formula Presented]
             collisions at [Formula Presented] TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {63},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2001},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.63.072001},
   Abstract = {We present the first measurement of the electron angular
             distribution parameter [Formula Presented] in [Formula
             Presented] events produced in proton-antiproton collisions
             as a function of the W boson transverse momentum. Our
             analysis is based on data collected using the DØ detector
             during the 1994–1995 Fermilab Tevatron run. We compare our
             results with next-to-leading order perturbative QCD, which
             predicts an angular distribution of [Formula Presented]
             where [Formula Presented] is the polar angle of the electron
             in the Collins-Soper frame. In the presence of QCD
             corrections, the parameters [Formula Presented] and [Formula
             Presented] become functions of [Formula Presented] the W
             boson transverse momentum. This measurement provides a test
             of next-to-leading order QCD corrections which are a
             non-negligible contribution to the W boson mass measurement.
             © 2001 The American Physical Society.},
   Doi = {10.1103/PhysRevD.63.072001},
   Key = {fds332356}
}

@article{fds308088,
   Author = {Collaboration, CDF},
   Title = {Measurement of the Associated ƒ× + ƒÝ„b Production
             Cross Section in pp Collisions at = 1.8 TeV},
   Journal = {Phys. Rev.},
   Volume = {D60},
   Number = {8},
   Pages = {092003},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/physrevlett.97.082004},
   Abstract = {We present a measurement of the top quark pair production
             cross section in pp collisions at square root of s = 1.96
             TeV using 318 pb(-1) of data collected with the Collider
             Detector at Fermilab. We select tt[over ] decays into the
             final states enu+jets and mu nu+ jets, in which at least one
             b quark from the t-quark decays is identified using a
             secondary vertex-finding algorithm. Assuming a top quark
             mass of 178 GeV/c2, we measure a cross section of 8.7 +/-
             0.9(stat)(-0.9)+1.1(syst) pb. We also report the first
             observation of tt[over ] with significance greater than
             5sigma in the subsample in which both b quarks are
             identified, corresponding to a cross section of
             10.1(-1.4)+1.6(stat)(-1.3)+2.0(syst) pb.},
   Doi = {10.1103/physrevlett.97.082004},
   Key = {fds308088}
}

@article{fds307568,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson,
             M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau,
             M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker,
             OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernhard, R and Bernius, C and Bernlochner,
             FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
             RN},
   Title = {Measurement of the azimuthal angle dependence of inclusive
             jet yields in Pb+Pb collisions at √(sNN)=2.76 TeV with the
             ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {15},
   Pages = {152301},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.111.152301},
   Abstract = {Measurements of the variation of inclusive jet suppression
             as a function of relative azimuthal angle, Δφ, with
             respect to the elliptic event plane provide insight into the
             path-length dependence of jet quenching. ATLAS has measured
             the Δφ dependence of jet yields in 0.14 nb(-1) of
             √(s(NN))=2.76 TeV Pb+Pb collisions at the LHC for jet
             transverse momenta p(T)>45 GeV in different collision
             centrality bins using an underlying event subtraction
             procedure that accounts for elliptic flow. The variation of
             the jet yield with Δφ was characterized by the parameter,
             v(2)(jet), and the ratio of out-of-plane (Δφ~π/2) to
             in-plane (Δφ~0) yields. Nonzero v(2)(jet) values were
             measured in all centrality bins for p(T)<160 GeV. The jet
             yields are observed to vary by as much as 20% between
             in-plane and out-of-plane directions.},
   Doi = {10.1103/physrevlett.111.152301},
   Key = {fds307568}
}

@article{fds310404,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abou
             Zeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amor’Os, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
             ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Measurement of the azimuthal anisotropy for charged particle
             production in √SNN = 2.76 TeV lead-lead
             collisions with the ATLAS detector},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {86},
   Number = {1},
   Pages = {014907-1-014907-41},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevC.86.014907},
   Abstract = {Differential measurements of charged particle azimuthal
             anisotropy are presented for lead-lead collisions at √sNN
             = 2.76 TeV with the ATLAS detector at the LHC, based on an
             integrated luminosity of approximately 8 μb− 1. This
             anisotropy is characterized via a Fourier expansion of the
             distribution of charged particles in azimuthal angle
             relative to the reaction plane, with the coefficients vn
             denoting the magnitude of the anisotropy. Significant
             v2–v6 values are obtained as a function of transverse
             momentum (0.5 < pT < 20 GeV), pseudorapidity (|η| < 2.5),
             and centrality using an event plane method. The vn values
             for n ≥ 3 are found to vary weakly with both η and
             centrality, and their pT dependencies are found to follow an
             approximate scaling relation, v1/nn (pT) ∝ v1/22 (pT),
             except in the top 5% most central collisions. A Fourier
             analysis of the charged particle pair distribution in
             relative azimuthal angle (Δϕ = ϕa − ϕb) is performed
             to extract the coefficients vn, n = (cos nΔϕ). For pairs
             of charged particles with a large pseudorapidity gap (|Δη
             = ηa − ηb| > 2) and one particle with pT < 3 GeV, the
             v2,2–v6,6 values are found to factorize as vn, n(paT, pbT)
             ≈ vn(paT)vn(pbT) in central and midcentral events. Such
             factorization suggests that these values of v2,2–v6,6 are
             primarily attributable to the response of the created matter
             to the fluctuations in the geometry of the initial state. A
             detailed study shows that the v1,1(paT, pbT) data are
             consistent with the combined contributions from a
             rapidity-even v1 and global momentum conservation.A
             two-component fit is used to extract the v1 contribution.
             The extracted v1 isobserved to cross zero at pT ≈ 1.0 GeV,
             reaches a maximum at 4–5 GeV with a value comparable to
             that for v3, and decreases at higher pT.},
   Doi = {10.1103/PhysRevC.86.014907},
   Key = {fds310404}
}

@article{fds347485,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
             M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
             E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
             M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
             KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
             U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
             D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
             BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
             S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V},
   Title = {Measurement of the azimuthal anisotropy of charged particles
             produced in s NN = 5.02 TeV Pb+Pb collisions with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {12},
   Pages = {997},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-6468-7},
   Abstract = {Measurements of the azimuthal anisotropy in lead-lead
             collisions at s NN = 5.02 TeV are presented using a data
             sample corresponding to 0.49 nb - 1 integrated luminosity
             collected by the ATLAS experiment at the LHC in 2015. The
             recorded minimum-bias sample is enhanced by triggers for
             "ultra-central" collisions, providing an opportunity to
             perform detailed study of flow harmonics in the regime where
             the initial state is dominated by fluctuations. The
             anisotropy of the charged-particle azimuthal angle
             distributions is characterized by the Fourier coefficients,
             v 2 - v 7 , which are measured using the two-particle
             correlation, scalar-product and event-plane methods. The
             goal of the paper is to provide measurements of the
             differential as well as integrated flow harmonics v n over
             wide ranges of the transverse momentum, 0.5  < p T <
              60 GeV, the pseudorapidity, | η | <  2.5, and the
             collision centrality 0-80%. Results from different methods
             are compared and discussed in the context of previous and
             recent measurements in Pb+Pb collisions at s NN = 2.76 
             TeV and 5.02  TeV . In particular, the shape of the p T
             dependence of elliptic or triangular flow harmonics is
             observed to be very similar at different centralities after
             scaling the v n and p T values by constant factors over the
             centrality interval 0-60% and the p T range 0.5  < p T <
              5 GeV.},
   Doi = {10.1140/epjc/s10052-018-6468-7},
   Key = {fds347485}
}

@article{fds349434,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA},
   Title = {Measurement of the azimuthal anisotropy of charged-particle
             production in Xe+Xe collisions at sNN =5.44 TeV with the
             ATLAS detector},
   Journal = {Physical Review C},
   Volume = {101},
   Number = {2},
   Year = {2020},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevC.101.024906},
   Abstract = {This paper describes the measurements of flow harmonics
             v2-v6 in 3μb-1 of Xe+Xe collisions at sNN=5.44 TeV
             performed using the ATLAS detector at the Large Hadron
             Collider (LHC). Measurements of the centrality,
             multiplicity, and pT dependence of the vn obtained using
             two-particle correlations and the scalar product technique
             are presented. The measurements are also performed using a
             template-fit procedure, which was developed to remove
             nonflow correlations in small collision systems. This
             nonflow removal is shown to have a significant influence on
             the measured vn at high pT, especially in peripheral events.
             Comparisons of the measured vn with measurements in Pb+Pb
             collisions and p+Pb collisions at sNN=5.02 TeV are also
             presented. The vn values in Xe+Xe collisions are observed to
             be larger than those in Pb+Pb collisions for n=2, 3, and 4
             in the most central events. However, with decreasing
             centrality or increasing harmonic order n, the vn values in
             Xe+Xe collisions become smaller than those in Pb+Pb
             collisions. The vn in Xe+Xe and Pb+Pb collisions are also
             compared as a function of the mean number of participating
             nucleons, (Npart), and the measured charged-particle
             multiplicity in the detector. The v3 values in Xe+Xe and
             Pb+Pb collisions are observed to be similar at the same
             (Npart) or multiplicity, but the other harmonics are
             significantly different. The ratios of the measured vn in
             Xe+Xe and Pb+Pb collisions, as a function of centrality, are
             also compared to theoretical calculations.},
   Doi = {10.1103/PhysRevC.101.024906},
   Key = {fds349434}
}

@article{fds307737,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the azimuthal ordering of charged hadrons
             with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.052005},
   Abstract = {This paper presents a study of the possible ordering of
             charged hadrons in the azimuthal angle relative to the beam
             axis in high-energy proton-proton collisions at the Large
             Hadron Collider (LHC). A spectral analysis of correlations
             between longitudinal and transverse components of the
             momentum of the charged hadrons, driven by the search for
             phenomena related to the structure of the QCD field, is
             performed. Data were recorded with the ATLAS detector at
             center-of-mass energies of √s=900GeV and √s=7TeV. The
             correlations measured in a kinematic region dominated by
             low-pT particles are not well described by conventional
             models of hadron production. The measured spectra show
             features consistent with the fragmentation of a QCD string
             represented by a helixlike ordered gluon chain. © 2012
             CERN.},
   Doi = {10.1103/PhysRevD.86.052005},
   Key = {fds307737}
}

@article{fds308126,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the b jet cross section in events with a Z
             boson in $p\bar{p}$ collisions at $\sqrt{s} =$
             1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D74},
   Number = {3},
   Pages = {032008},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.74.032008},
   Abstract = {A measurement of the inclusive bottom jet cross section is
             presented for events containing a Z boson in p anti-p
             collisions at s**(1/2) = 1.96 TeV using the Collider
             Detector at Fermilab. Z bosons are identified in their
             electron and muon decay modes, and b jets with E(t) > 20 GeV
             and |eta| l+ l-) = 0.93 +/- 0.36 pb is found, where B(Z -->
             l+ l-) is the branching ratio of the Z boson or gamma* into
             a single flavor dilepton pair (e or mu) in the mass range
             between 66 and 116 GeV/c2. The ratio of b jets to the total
             number of jets of any flavor in the Z sample, within the
             same kinematic range as the b jets, is 2.36 +/- 0.92\%.
             Here, the uncertainties are the quadratic sum of statistical
             and systematic uncertainties. Predictions made with NLO QCD
             agree, within experimental and theoretical uncertainties,
             with these measurements.},
   Doi = {10.1103/PhysRevD.74.032008},
   Key = {fds308126}
}

@article{fds307827,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
             M and de Barbaro, P and De Cecco and S and Deisher, A and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, H-C and Farrington, S and Feindt,
             M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis,
             E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu,
             T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck,
             J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak,
             R and Maeshima, K and Makhoul, K and Maksimovic, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan,
             N and Redondo, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel,
             S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki,
             M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
             P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner,
             RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters,
             D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T},
   Title = {Measurement of the B(s)0 lifetime in fully and partially
             reconstructed B(s)0→D(s)(-)(ϕπ(-))X decays in p¯p
             collisions at √s=1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {107},
   Number = {27},
   Pages = {272001},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.107.272001},
   Abstract = {We present a measurement of the B(s)(0) lifetime in fully
             and partially reconstructed B(s)(0)→D(s)(-)(ϕπ(-))X
             decays in 1.3  fb(-1) collected in pp ¯ collisions at
             √s=1.96 TeV by the CDF II detector at the Fermilab
             Tevatron. We measure τ(B(s)(0))=1.518±0.041(stat)±0.027(syst)  ps.
             The ratio of this result and the world average B(0) lifetime
             yields τ(B(s)(0))/τ(B(0))=0.99±0.03, which is in
             agreement with recent theoretical predictions.},
   Doi = {10.1103/physrevlett.107.272001},
   Key = {fds307827}
}

@article{fds308079,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the B+ production cross section in p anti-p
             collisions at s**(1/2) = 1960-GeV},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {5},
   Pages = {012010},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.052001},
   Abstract = {We present a new measurement of the B+ meson differential
             cross section dsigma/dpT at sqrt(s)=1960 GeV. The data
             correspond to an integrated luminosity of 739 pb-1 collected
             with the upgraded CDF detector (CDF II) at the Fermilab
             Tevatron collider. B+ candidates are reconstructed through
             the decay B+-->J/psiK+, with J/psi-->µ+µ-. The integrated
             cross section for producing B+ mesons with pT>=6 GeV/c and
             |y|},
   Doi = {10.1103/PhysRevD.93.052001},
   Key = {fds308079}
}

@article{fds307787,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel,
             M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
             M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
             T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins,
             NJ and Collins-Tooth, C and Collot, J},
   Title = {Measurement of the b-hadron production cross section using
             decays to D *+μ -X final states in pp
             collisions at √s = 7 TeV with the ATLAS
             detector},
   Journal = {Nuclear Physics B},
   Volume = {864},
   Number = {3},
   Pages = {341-381},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.nuclphysb.2012.07.009},
   Abstract = {The b-hadron production cross section is measured with the
             ATLAS detector in pp collisions at s=7TeV, using 3.3pb -1 of
             integrated luminosity, collected during the 2010 LHC run.
             The b-hadrons are selected by partially reconstructing D
             z.ast;+μ -X final states. Differential cross sections are
             measured as functions of the transverse momentum and
             pseudorapidity. The measured production cross section for a
             b-hadron with p T&gt;9GeV and |n|&lt;2.5 is
             32.7±0.8(stat.)-6.8+4.5(syst.)μb, higher than the
             next-to-leading-order QCD predictions but consistent within
             the experimental and theoretical uncertainties. ©
             2012.},
   Doi = {10.1016/j.nuclphysb.2012.07.009},
   Key = {fds307787}
}

@article{fds307987,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the b-hadron production cross section using
             decays to mu[sup -]D[sup 0]X final states in p[overline p]
             collisions at sqrt(s) = 1.96 TeV},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {9},
   Pages = {092003},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.092003},
   Abstract = {We report a measurement of the production cross section for
             b hadrons in pp̄ collisions at s=1.96TeV. Using a data
             sample derived from an integrated luminosity of 83pb-1
             collected with the upgraded Collider Detector (CDF II) at
             the Fermilab Tevatron, we analyze b hadrons, Hb, partially
             reconstructed in the semileptonic decay mode Hb→μ-D0X.
             Our measurement of the inclusive production cross section
             for b hadrons with transverse momentum pT>9GeV/c and
             rapidity |y|<0.6 is σ=1.30μb±0.05μb(stat)±0.
             14μb(syst)±0.07μb(B), where the uncertainties are
             statistical, systematic, and from branching fractions,
             respectively. The differential cross sections dσ/dpT are
             found to be in good agreement with recent measurements of
             the Hb cross section and well described by fixed-order
             next-to-leading logarithm predictions. © 2009 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.79.092003},
   Key = {fds307987}
}

@article{fds361246,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the B/s0 anti-B/s0 oscillation
             frequency},
   Journal = {Phys. Rev. Lett.},
   Volume = {97},
   Number = {191802},
   Pages = {062003},
   Year = {2006},
   Abstract = {We measure the masses of $b$ hadrons in exclusively
             reconstructed final states containing a $J/\psi\to\mu^-\mu^+$
             decay using $\rm 220 pb^{-1}$ of data collected by the CDF
             II experiment. We find: m(B^+) = 5279.10 \pm 0.41_{(stat.)}
             \pm 0.36_{(sys.)} MeVcc, m(B^0) = 5279.63 \pm 0.53_{(stat.)}
             \pm 0.33_{(sys.)} MeVcc, m(B^0_s) = 5366.01 \pm
             0.73_{(stat.)} \pm 0.33_{(sys.)} MeVcc, m(\Lambda^0_b) =
             5619.7 \pm 1.2_{(stat.)} \pm 1.2_{(sys.)} MeVcc. m(B^+) -
             m(B^0) = -0.53 \pm 0.67_{(stat.)} \pm 0.14_{(sys.)} MeVcc,
             m(B^0_s) - m(B^0) = 86.38 \pm 0.90_{(stat.)} \pm
             0.06_{(sys.)} MeVcc m(\Lambda^0_b) - m(B^0) = 339.2 \pm
             1.4_{(stat.)} \pm 0.1_{(sys.)} MeVcc. The measurements of
             the $B^0_s$, $\Lambda^0_b$ mass, $m(B^0_s)-m(B^0)$ and
             $m(\Lambda^0_b)-m(B^0)$ mass difference are of better
             precision than the current world averages.},
   Key = {fds361246}
}

@article{fds362145,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro,
             A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cresciolo, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
             PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Devlin, T and Dionisi, C and Dittmann, JR and DiTuro, P and Dorr, C and Donati, S and Donega, M and Dong, P and Donini,
             J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
             M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
             LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
             JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris, N and Giolo, K and Giordani, M and Giromini,
             P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos,
             G and Goncharov, M and Gonzalez, O and Gorelov, I and Goshaw, AT and Gotra,
             Y and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Hahn, K and Halkiadakis,
             E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Heijboer, A and Heinemann,
             B and Heinrich, J and Herndon, M and Hidas, D and Hill, CS and Hirschbuehl,
             D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela, J and Introzzi,
             G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon,
             T and Kang, J and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee,
             SW and Lefevre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister,
             A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
             M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
             H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto,
             A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mulmenstadt, J and Mukherjee, A and Muller, T and Mumford, R and Murat,
             P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg,
             K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou,
             V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel,
             NV and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
             L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli,
             S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
             A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P},
   Title = {Measurement of the Bc+ meson lifetime using the decay mode
             Bc+→J/ψe+νe},
   Journal = {Physical Review Letters},
   Volume = {97},
   Number = {1},
   Pages = {012002},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevLett.97.012002},
   Abstract = {We present a measurement of the Bc+ meson lifetime in the
             decay mode Bc+→J/ψe+νe using the Collider Detector at
             Fermilab II detector at the Fermilab Tevatron Collider. From
             a sample of about 360pb-1 of pp̄ collisions at s=1.96TeV,
             we reconstruct J/ψe+ pairs with invariant mass in the
             kinematically allowed range 4&lt;MJ/ψe&lt;6GeV/c2. A fit to
             the decay-length distribution of 238 signal events yields a
             measured Bc+ meson lifetime of 0.463+0.073-0.065(stat)±0.036(syst)ps.
             © 2006 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.97.012002},
   Key = {fds362145}
}

@article{fds307641,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'Errico, M},
   Title = {Measurement of the Bc-meson lifetime in the decay
             Bc-→J/ψπ},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.011101},
   Abstract = {The lifetime of the Bc- meson is measured using 272
             exclusive Bc-→J/ψ(→μ+μ-)π- decays reconstructed in
             data from proton-antiproton collisions corresponding to an
             integrated luminosity of 6.7 fb-1 recorded by the CDF II
             detector at the Fermilab Tevatron. The lifetime of the Bc-
             meson is measured to be τ(Bc-)=0.452±0.048(stat)±0.027(syst)
             ps. This is the first measurement of the Bc- meson lifetime
             in a fully reconstructed hadronic channel, and it agrees
             with previous results and has comparable precision. © 2013
             American Physical Society.},
   Doi = {10.1103/PhysRevD.87.011101},
   Key = {fds307641}
}

@article{fds307679,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grillo, L and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of the bottom-strange meson mixing phase in the
             full CDF data set.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {17},
   Pages = {171802},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.109.171802},
   Abstract = {We report a measurement of the bottom-strange meson mixing
             phase β(s) using the time evolution of B(s)(0)→J/ψ(→μ(+)μ(-))φ(→K(+)K(-))
             decays in which the quark-flavor content of the
             bottom-strange meson is identified at production. This
             measurement uses the full data set of proton-antiproton
             collisions at √s=1.96 TeV collected by the Collider
             Detector experiment at the Fermilab Tevatron, corresponding
             to 9.6 fb(-1) of integrated luminosity. We report confidence
             regions in the two-dimensional space of β(s) and the
             B(s)(0) decay-width difference ΔΓ(s) and measure
             β(s)∈[-π/2,-1.51]∪[-0.06,0.30]∪[1.26,π/2] at the
             68% confidence level, in agreement with the standard model
             expectation. Assuming the standard model value of β(s), we
             also determine ΔΓ(s)=0.068±0.026(stat)±0.009(syst)
             ps(-1) and the mean B(s)(0) lifetime τ(s)=1.528±0.019(stat)±0.009(syst)
             ps, which are consistent and competitive with determinations
             by other experiments.},
   Doi = {10.1103/physrevlett.109.171802},
   Key = {fds307679}
}

@article{fds307817,
   Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
             J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli,
             M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi,
             R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
             DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and Barbaro, PD and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F and D'errico, M and Canto, AD and Ruzza, BD and Dittmann, JR and D'onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan,
             G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giakoumopoulou,
             V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
             K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
             M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro,
             P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, C and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and Mcfarland, KS and Mcintyre, P and Mcnulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh,
             SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Poukhov,
             O and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro,
             A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Squillacioti, P and Stancari, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel,
             M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, WM and Yeh, GP and Yi, K and Yoh,
             J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zucchelli, S},
   Title = {Measurement of the branching fraction B(Λb0→Λc+π
             -π +π -) at
             CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.032003},
   Abstract = {We report an analysis of the Λb0→Λc+π -π +π - decay
             in a data sample collected by the CDF II detector at the
             Fermilab Tevatron corresponding to 2.4fb -1 of integrated
             luminosity. We reconstruct the currently largest samples of
             the decay modes Λb0→Λ c(2595) +π - (with Λ c(2595)
             +→Λc+π +π -), Λb0→Λ c(2625) +π - (with Λ c(2625)
             +→Λc+π +π -), Λb0→Σ c(2455) ++π -π - (with Σ
             c(2455) ++→Λc+π +), and Λb0→Σ c(2455)0π +π - (with
             Σ c(2455)0→Λc+π -) and measure the branching fractions
             relative to the Λb0→Λc+π - branching fraction. We
             measure the ratio B(Λb0→Λc+π -π +π -)/B(Λb0→Λc+π
             -)=3.04±0.33(stat)-0.55+0.70(syst) which is used to derive
             B(Λb0→Λc+π -π +π -)= (26.8-11.2+11.9)×10 -3. © 2012
             American Physical Society.},
   Doi = {10.1103/PhysRevD.85.032003},
   Key = {fds307817}
}

@article{fds313605,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of the branching ratio Γ(Λb0→ψ(2S)Λ0)/Γ(Λb0→J/ψΛ0)
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {751},
   Pages = {63-80},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {December},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.10.009},
   Abstract = {An observation of the Λb0→ψ(2S)Λ0 decay and a
             comparison of its branching fraction with that of the
             Λb0→J/ψΛ0 decay has been made with the ATLAS detector
             in proton–proton collisions at s=8 TeV at the LHC using an
             integrated luminosity of 20.6 fb−1. The J/ψ and ψ(2S)
             mesons are reconstructed in their decays to a muon pair,
             while the Λ0→pπ− decay is exploited for the Λ0 baryon
             reconstruction. The Λb0 baryons are reconstructed with
             transverse momentum pT>10 GeV and pseudorapidity |η|<2.1.
             The measured branching ratio of the Λb0→ψ(2S)Λ0 and
             Λb0→J/ψΛ0 decays is Γ(Λb0→ψ(2S)Λ0)/Γ(Λb0→J/ψΛ0)=0.501±0.033(stat)±0.019(syst),
             lower than the expectation from the covariant quark
             model.},
   Doi = {10.1016/j.physletb.2015.10.009},
   Key = {fds313605}
}

@article{fds310394,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai,
             Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
             FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
             MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov,
             AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
             JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
             S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
             IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Measurement of the centrality and pseudorapidity dependence
             of the integrated elliptic flow in lead-lead collisions at
             [Formula: see text] TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {8},
   Pages = {2982},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-2982-4},
   Abstract = {The integrated elliptic flow of charged particles produced
             in Pb+Pb collisions at [Formula: see text] TeV has been
             measured with the ATLAS detector using data collected at the
             Large Hadron Collider. The anisotropy parameter, [Formula:
             see text], was measured in the pseudorapidity range
             [Formula: see text] with the event-plane method. In order to
             include tracks with very low transverse momentum [Formula:
             see text], thus reducing the uncertainty in [Formula: see
             text] integrated over [Formula: see text], a [Formula: see
             text] data sample recorded without a magnetic field in the
             tracking detectors is used. The centrality dependence of the
             integrated [Formula: see text] is compared to other
             measurements obtained with higher [Formula: see text]
             thresholds. The integrated elliptic flow is weakly
             decreasing with [Formula: see text]. The integrated
             [Formula: see text] transformed to the rest frame of one of
             the colliding nuclei is compared to the lower-energy RHIC
             data.},
   Doi = {10.1140/epjc/s10052-014-2982-4},
   Key = {fds310394}
}

@article{fds307764,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Measurement of the centrality dependence of the charged
             particle pseudorapidity distribution in lead-lead collisions
             at √s NN=2.76 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {710},
   Number = {3},
   Pages = {363-382},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.045},
   Abstract = {The ATLAS experiment at the LHC has measured the centrality
             dependence of charged particle pseudorapidity distributions
             over |η|<2 in lead-lead collisions at a nucleon-nucleon
             centre-of-mass energy of √s NN=2.76 TeV. In order to
             include particles with transverse momentum as low as 30 MeV,
             the data were recorded with the central solenoid magnet off.
             Charged particles were reconstructed with two algorithms
             (2-point "tracklets" and full tracks) using information from
             the pixel detector only. The lead-lead collision centrality
             was characterized by the total transverse energy in the
             forward calorimeter in the range 3.2<|η|<4.9. Measurements
             are presented of the per-event charged particle
             pseudorapidity distribution, dN ch/dη, and the average
             charged particle multiplicity in the pseudorapidity interval
             |η|<0.5 in several intervals of collision centrality. The
             results are compared to previous mid-rapidity measurements
             at the LHC and RHIC. The variation of the mid-rapidity
             charged particle yield per colliding nucleon pair with the
             number of participants is consistent with lower sNN results.
             The shape of the dN ch/dη distribution is found to be
             independent of centrality within the systematic
             uncertainties of the measurement. © 2012
             CERN.},
   Doi = {10.1016/j.physletb.2012.02.045},
   Key = {fds307764}
}

@article{fds315363,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arguin, J-F and Argyropoulos,
             S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
             G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
             P and Balli, F and Banas, E and Banerjee, S and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
             N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
             R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
             FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
             MI and Besjes, GJ and Bessidskaia Bylund and O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho
             Toro, R and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa,
             A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo
             Gimenez, V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
             B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavez
             Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
             IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Coggeshall, J and Cole, B and Cole, S and Colijn, AP and Collins-Tooth, C and Collot, J and Colombo,
             T},
   Title = {Measurement of the centrality dependence of the
             charged-particle pseudorapidity distribution in proton-lead
             collisions at [Formula: see text] TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {4},
   Pages = {199},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4002-3},
   Abstract = {The centrality dependence of the mean charged-particle
             multiplicity as a function of pseudorapidity is measured in
             approximately 1 [Formula: see text]b[Formula: see text] of
             proton-lead collisions at a nucleon-nucleon centre-of-mass
             energy of [Formula: see text] [Formula: see text] using the
             ATLAS detector at the Large Hadron Collider. Charged
             particles with absolute pseudorapidity less than 2.7 are
             reconstructed using the ATLAS pixel detector. The [Formula:
             see text] collision centrality is characterised by the total
             transverse energy measured in the Pb-going direction of the
             forward calorimeter. The charged-particle pseudorapidity
             distributions are found to vary strongly with centrality,
             with an increasing asymmetry between the proton-going and
             Pb-going directions as the collisions become more central.
             Three different estimations of the number of nucleons
             participating in the [Formula: see text] collision have been
             carried out using the Glauber model as well as two
             Glauber-Gribov inspired extensions to the Glauber model.
             Charged-particle multiplicities per participant pair are
             found to vary differently for these three models,
             highlighting the importance of including colour fluctuations
             in nucleon-nucleon collisions in the modelling of the
             initial state of [Formula: see text] collisions.},
   Doi = {10.1140/epjc/s10052-016-4002-3},
   Key = {fds315363}
}

@article{fds376310,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Aktas, S and Al Khoury and K and Alberghi,
             GL and Albert, J and Albicocco, P and Albouy, GL and Alderweireldt, S and Alegria, ZL and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
             Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
             C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
             M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
             SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arbiol Val and SJ and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling,
             J-H and Arnaez, O and Arnold, H and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atmani, H and Atmasiddha,
             PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Baer, TM and Bagnaia, P and Bahmani, M and Bahner, D and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Baker, OK and Bakos, E and Bakshi Gupta and D and Balakrishnan, V and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barel, MZ and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau, T and Beaucamp, JY and Beauchemin, PH and Becherer, F and Bechtle, P and Beck,
             HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berrocal Guardia and A and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhalla, NK and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Biryukov, S and Bisanz, T and Bisceglie, E and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
             V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
             R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
             PA and Brüers, B and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
             AR and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai,
             Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carducci, G and Carli, T and Carlino, G and Carlotto, JI and Carlson,
             BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos,
             F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castillo,
             FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cepaitis, V and Cerny, K and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chakraborty, D and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi,
             K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Clark, A},
   Title = {Measurement of the Centrality Dependence of the Dijet Yield
             in p+Pb Collisions at sqrt[s_{NN}]=8.16  TeV with the
             ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {132},
   Number = {10},
   Pages = {102301},
   Year = {2024},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.132.102301},
   Abstract = {ATLAS measured the centrality dependence of the dijet yield
             using 165  nb^{-1} of p+Pb data collected at
             sqrt[s_{NN}]=8.16  TeV in 2016. The event centrality,
             which reflects the p+Pb impact parameter, is characterized
             by the total transverse energy registered in the Pb-going
             side of the forward calorimeter. The central-to-peripheral
             ratio of the scaled dijet yields, R_{CP}, is evaluated, and
             the results are presented as a function of variables that
             reflect the kinematics of the initial hard parton scattering
             process. The R_{CP} shows a scaling with the Bjorken x of
             the parton originating from the proton, x_{p}, while no such
             trend is observed as a function of x_{Pb}. This analysis
             provides unique input to understanding the role of small
             proton spatial configurations in p+Pb collisions by covering
             parton momentum fractions from the valence region down to
             x_{p}∼10^{-3} and x_{Pb}∼4×10^{-4}.},
   Doi = {10.1103/physrevlett.132.102301},
   Key = {fds376310}
}

@article{fds310286,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Measurement of the charge asymmetry in dileptonic decays of
             top quark pairs in pp collisions at √s = 7 TeV using the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2015)061},
   Abstract = {A measurement of the top-antitop (tt¯) charge asymmetry is
             presented using data corresponding to an integrated
             luminosity of 4.6 fb−1 of LHC pp collisions at a
             centreof-mass energy of 7 TeV collected by the ATLAS
             detector. Events with two charged leptons, at least two jets
             and large missing transverse momentum are selected. Two
             observables are studied: ACℓℓ based on the identified
             charged leptons, and (Formula Presented.), based on the
             reconstructed tt final state. The asymmetries are measured
             to be (Formula Presented.). The measured values are in
             agreement with the Standard Model predictions.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP05(2015)061},
   Key = {fds310286}
}

@article{fds356770,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A},
   Title = {Measurement of the charge asymmetry in highly boosted
             top-quark pair production in √s=8 TeV pp collision data
             collected by the ATLAS experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {756},
   Pages = {52-71},
   Year = {2016},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.02.055},
   Abstract = {In the pp→tt¯ process the angular distributions of top
             and anti-top quarks are expected to present a subtle
             difference, which could be enhanced by processes not
             included in the Standard Model. This Letter presents a
             measurement of the charge asymmetry in events where the
             top-quark pair is produced with a large invariant mass. The
             analysis is performed on 20.3 fb−1 of pp collision data at
             s=8TeV collected by the ATLAS experiment at the LHC, using
             reconstruction techniques specifically designed for the
             decay topology of highly boosted top quarks. The charge
             asymmetry in a fiducial region with large invariant mass of
             the top-quark pair (mtt¯>0.75 TeV) and an absolute rapidity
             difference of the top and anti-top quark candidates within
             −2<|yt|−|yt¯|<2 is measured to be 4.2±3.2%, in
             agreement with the Standard Model prediction at
             next-to-leading order. A differential measurement in three
             tt¯ mass bins is also presented.},
   Doi = {10.1016/j.physletb.2016.02.055},
   Key = {fds356770}
}

@article{fds307729,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati,
             S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard,
             R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli,
             F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji,
             W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi,
             M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland,
             W},
   Title = {Measurement of the charge asymmetry in top quark pair
             production in pp collisions at [Formula: see text]
             using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {72},
   Number = {6},
   Pages = {2039},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2039-5},
   Abstract = {A measurement of the top-antitop production charge asymmetry
             <i>A</i><sub><i>C</i></sub> is presented using data
             corresponding to an integrated luminosity of 1.04
             fb<sup>-1</sup> of <i>pp</i> collisions at [Formula: see
             text] TeV collected by the ATLAS detector at the LHC.
             Events are selected with a single lepton (electron or muon),
             missing transverse momentum and at least four jets of which
             at least one jet is identified as coming from a
             <i>b</i>-quark. A kinematic fit is used to reconstruct the
             [Formula: see text] event topology. After background
             subtraction, a Bayesian unfolding procedure is performed to
             correct for acceptance and detector effects. The measured
             value of <i>A</i><sub><i>C</i></sub> is [Formula: see text],
             consistent with the prediction from the MC@NLO Monte Carlo
             generator of <i>A</i><sub><i>C</i></sub> =0.006±0.002.
             Measurements of <i>A</i><sub><i>C</i></sub> in two ranges of
             invariant mass of the top-antitop pair are also
             shown.},
   Doi = {10.1140/epjc/s10052-012-2039-5},
   Key = {fds307729}
}

@article{fds372122,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V},
   Title = {Measurement of the charge asymmetry in top-quark pair
             production in association with a photon with the ATLAS
             experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {843},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.137848},
   Abstract = {A measurement of the charge asymmetry in top-quark pair
             (tt¯) production in association with a photon is presented.
             The measurement is performed in the single-lepton tt¯ decay
             channel using proton–proton collision data collected with
             the ATLAS detector at the Large Hadron Collider at CERN at a
             centre-of-mass-energy of 13 TeV during the years
             2015–2018, corresponding to an integrated luminosity of
             139 fb−1. The charge asymmetry is obtained from the
             distribution of the difference of the absolute rapidities of
             the top quark and antiquark using a profile likelihood
             unfolding approach. It is measured to be AC=−0.003±0.029
             in agreement with the Standard Model expectation.},
   Doi = {10.1016/j.physletb.2023.137848},
   Key = {fds372122}
}

@article{fds323672,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
             M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
             C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biesuz,
             NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard,
             CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho
             Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman,
             JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
             S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
             K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
   Title = {Measurement of the charge asymmetry in top-quark pair
             production in the lepton-plus-jets final state in pp
             collision data at [Formula: see text] with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {87},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-3910-6},
   Abstract = {This paper reports inclusive and differential measurements
             of the [Formula: see text] charge asymmetry [Formula: see
             text] in [Formula: see text] of [Formula: see text][Formula:
             see text] collisions recorded by the ATLAS experiment at the
             Large Hadron Collider at CERN. Three differential
             measurements are performed as a function of the invariant
             mass, transverse momentum and longitudinal boost of the
             [Formula: see text] system. The [Formula: see text] pairs
             are selected in the single-lepton channels (<i>e</i> or
             [Formula: see text]) with at least four jets, and a
             likelihood fit is used to reconstruct the [Formula: see
             text] event kinematics. A Bayesian unfolding procedure is
             performed to infer the asymmetry at parton level from the
             observed data distribution. The inclusive [Formula: see
             text] charge asymmetry is measured to be [Formula: see text]
             (stat. [Formula: see text] syst.). The inclusive and
             differential measurements are compatible with the values
             predicted by the Standard Model.},
   Doi = {10.1140/epjc/s10052-016-3910-6},
   Key = {fds323672}
}

@article{fds347519,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
             Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
             De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
             TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN},
   Title = {Measurement of the charged-particle multiplicity inside jets
             from [Formula: see text][Formula: see text] pp
             collisions with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {6},
   Pages = {322},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4126-5},
   Abstract = {The number of charged particles inside jets is a widely used
             discriminant for identifying the quark or gluon nature of
             the initiating parton and is sensitive to both the
             perturbative and non-perturbative components of
             fragmentation. This paper presents a measurement of the
             average number of charged particles with [Formula: see text]
             [Formula: see text] inside high-momentum jets in dijet
             events using 20.3 fb[Formula: see text] of data recorded
             with the ATLAS detector in <i>pp</i> collisions at [Formula:
             see text] [Formula: see text] collisions at the LHC. The
             jets considered have transverse momenta from 50 [Formula:
             see text] up to and beyond 1.5 [Formula: see text]. The
             reconstructed charged-particle track multiplicity
             distribution is unfolded to remove distortions from detector
             effects and the resulting charged-particle multiplicity is
             compared to several models. Furthermore, quark and gluon jet
             fractions are used to extract the average charged-particle
             multiplicity for quark and gluon jets separately.},
   Doi = {10.1140/epjc/s10052-016-4126-5},
   Key = {fds347519}
}

@article{fds313619,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Akesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of the correlation between flow harmonics of
             different order in lead-lead collisions at √sNN
             = 2.76 TeV with the ATLAS detector},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {92},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   ISSN = {0556-2813},
   url = {http://dx.doi.org/10.1103/PhysRevC.92.034903},
   Abstract = {Correlations between the elliptic or triangular flow
             coefficients vm (m = 2 or 3) and other flow harmonics vn (n
             = 2 to 5) are measured using √sNN = 2.76 TeV Pb + Pb
             collision data collected in 2010 by the ATLAS experiment at
             the LHC, corresponding to an integrated luminosity of 7
             μb−1. The vm-vn correlations are measured in midrapidity
             as a function of centrality, and, for events within the same
             centrality interval, as a function of event ellipticity or
             triangularity defined in a forward rapidity region. For
             events within the same centrality interval, v3 is found to
             be anticorrelated with v2 and this anticorrelation is
             consistent with similar anticorrelations between the
             corresponding eccentricities, ∊2 and ∊3. However, it is
             observed that v4 increases strongly with v2, and v5
             increases strongly with both v2 and v3. The trend and
             strength of the vm-vn correlations for n = 4 and 5 are found
             to disagree with ∊m-∊n correlations predicted by
             initial-geometry models. Instead, these correlations are
             found to be consistent with the combined effects of a linear
             contribution to vn and a nonlinear term that is a function
             of v22 or of v2v3, as predicted by hydrodynamic models. A
             simple two-component fit is used to separate these two
             contributions. The extracted linear and nonlinear
             contributions to v4 and v5 are found to be consistent with
             previously measured event-plane correlations.},
   Doi = {10.1103/PhysRevC.92.034903},
   Key = {fds313619}
}

@article{fds356785,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Measurement of the correlation between the polar angles of
             leptons from top quark decays in the helicity basis at s =7
             T e V using the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {1},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.012002},
   Abstract = {A measurement of the correlations between the polar angles
             of leptons from the decay of pair-produced t and t¯ quarks
             in the helicity basis is reported, using proton-proton
             collision data collected by the ATLAS detector at the LHC.
             The dataset corresponds to an integrated luminosity of 4.6
             fb-1 at a center-of-mass energy of s=7 TeV collected during
             2011. Candidate events are selected in the dilepton topology
             with large missing transverse momentum and at least two
             jets. The angles θ1 and θ2 between the charged leptons and
             the direction of motion of the parent quarks in the tt¯
             rest frame are sensitive to the spin information, and the
             distribution of cosθ1·cosθ2 is sensitive to the spin
             correlation between the t and t¯ quarks. The distribution
             is unfolded to parton level and compared to the
             next-to-leading order prediction. A good agreement is
             observed.},
   Doi = {10.1103/PhysRevD.93.012002},
   Key = {fds356785}
}

@article{fds374216,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
             A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
             MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames,
             CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche,
             CS and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena,
             E},
   Title = {Measurement of the CP properties of Higgs boson interactions
             with τ -leptons with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {7},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2023},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11583-y},
   Abstract = {A study of the charge conjugation and parity (CP) properties
             of the interaction between the Higgs boson and τ -leptons
             is presented. The study is based on a measurement of CP
             -sensitive angular observables defined by the visible decay
             products of τ -leptons produced in Higgs boson decays. The
             analysis uses 139 fb- 1of proton–proton collision data
             recorded at a centre-of-mass energy of s=13 TeV with the
             ATLAS detector at the Large Hadron Collider. Contributions
             from CP -violating interactions between the Higgs boson and
             τ -leptons are described by a single mixing angle parameter
             ϕτin the generalised Yukawa interaction. Without
             constraining the H→ ττ signal strength to its expected
             value under the Standard Model hypothesis, the mixing angle
             ϕτis measured to be 9∘± 16∘, with an expected value
             of 0∘± 28∘at the 68% confidence level. The pure CP -odd
             hypothesis is disfavoured at a level of 3.4 standard
             deviations. The results are compatible with the predictions
             for the Higgs boson in the Standard Model.},
   Doi = {10.1140/epjc/s10052-023-11583-y},
   Key = {fds374216}
}

@article{fds307807,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Bousson, N and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
             A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
             ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De Barbaro and P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F},
   Title = {Measurement of the CP-violating phase βsJ/ψ in Bs0→J/ψ
             decays with the CDF II detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.072002},
   Abstract = {We present a measurement of the CP-violating parameter
             βsJ/ψ using approximately 6500 Bs0→J/ψ decays
             reconstructed with the CDF II detector in a sample of pp̄
             collisions at √s=1.96TeV corresponding to 5.2fb -1
             integrated luminosity produced by the Tevatron collider at
             Fermilab. We find the CP-violating phase to be within the
             range βsJ/ψ [0.02,0.52] [1.08,1.55] at 68% confidence
             level where the coverage property of the quoted interval is
             guaranteed using a frequentist statistical analysis. This
             result is in agreement with the standard model expectation
             at the level of about one Gaussian standard deviation. We
             consider the inclusion of a potential S-wave contribution to
             the Bs0→J/ψK +K - final state which is found to be
             negligible over the mass interval 1.009<m(K +K
             -)<1.028GeV/c2. Assuming the standard model prediction for
             the CP-violating phase βsJ/ψ, we find the Bs0 decay width
             difference to be ΔΓ s=0.075±0.035(stat) ±0.006(syst)ps
             -1. We also present the most precise measurements of the Bs0
             mean lifetime τ(Bs0)=1.529±0.025(stat) ±0.012(syst)ps,
             the polarization fractions |A 0(0)|2=0. 524±0.013(stat)±0.015(syst)
             and |A -(0)|2=0. 231±0.014(stat)±0.015(syst), as well as
             the strong phase δ -=2.95±0.64(stat)±0.07(syst)rad. In
             addition, we report an alternative Bayesian analysis that
             gives results consistent with the frequentist approach. ©
             2012 American Physical Society.},
   Doi = {10.1103/PhysRevD.85.072002},
   Key = {fds307807}
}

@article{fds356106,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
             L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
             JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA},
   Title = {Measurement of the CP-violating phase ϕs in
             Bs0→J/ψϕ decays in ATLAS at 13 TeV},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {4},
   Year = {2021},
   Month = {April},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09011-0},
   Abstract = {A measurement of the Bs0→J/ψϕ decay parameters using
             80.5fb-1 of integrated luminosity collected with the ATLAS
             detector from 13 Te proton–proton collisions at the LHC
             is presented. The measured parameters include the
             CP-violating phase ϕs, the width difference Δ Γ s between
             the Bs0 meson mass eigenstates and the average decay width
             Γ s. The values measured for the physical parameters are
             combined with those from 19.2fb-1 of 7 and 8 Te data,
             leading to the following: ϕs=-0.087±0.036(stat.)±0.021(syst.)radΔΓs=0.0657±0.0043(stat.)±0.0037(syst.)ps-1Γs=0.6703±0.0014(stat.)±0.0018(syst.)ps-1Results
             for ϕs and Δ Γ s are also presented as 68% confidence
             level contours in the ϕs–Δ Γ s plane. Furthermore the
             transversity amplitudes and corresponding strong phases are
             measured. ϕs and Δ Γ s measurements are in agreement with
             the Standard Model predictions.},
   Doi = {10.1140/epjc/s10052-021-09011-0},
   Key = {fds356106}
}

@article{fds321112,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Measurement of the CP-violating phase ϕsand the
             Bs0meson decay width difference with
             Bs0→ J/ψϕ decays in
             ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2016)147},
   Abstract = {A measurement of the Bs0decay parameters in the Bs0→
             J/ψϕ channel using an integrated luminosity of 14.3
             fb−1collected by the ATLAS detector from 8 TeV pp
             collisions at the LHC is presented. The measured parameters
             include the CP -violating phase ϕs, the decay width Γs and
             the width difference between the mass eigenstates ΔΓs. The
             values measured for the physical parameters are
             statistically combined with those from 4.9 fb−1of 7 TeV
             data, leading to the following: Φs = -0.090 ± 0.078
             (stat.) ± (syst.) rad Δ Γs = 0.085 ± 0.011 (stat.) ±
             0.007 (syst.) Ps-1 Δ Γs = 0.675 ± 0.003 (stat.) ± 0.03
             (syst.) Ps-1 In the analysis the parameter ΔΓs is
             constrained to be positive. Results for ϕs and ΔΓs are
             also presented as 68% and 95% likelihood contours in the
             ϕs-ΔΓs plane. Also measured in this decay channel are the
             transversity amplitudes and corresponding strong phases. All
             measurements are in agreement with the Standard Model
             predictions.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP08(2016)147},
   Key = {fds321112}
}

@article{fds307594,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and d'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucà, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
             N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of the cross section for direct-photon
             production in association with a heavy quark in pp[over ¯]
             collisions at sqrt[s]=1.96  TeV.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {4},
   Pages = {042003},
   Year = {2013},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.111.042003},
   Abstract = {We report on a measurement of the cross section for
             direct-photon production in association with a heavy quark
             using the full data set of sqrt[s]=1.96  TeV
             proton-antiproton collisions corresponding to 9.1  fb-1
             of integrated luminosity collected by the CDF II detector at
             the Fermilab Tevatron. The measurements are performed as a
             function of the photon transverse momentum, covering a
             photon transverse momentum between 30 and 300 GeV, photon
             rapidities |yγ|<1.0, a heavy-quark-jet transverse momentum
             pTjet>20  GeV, and jet rapidities |yjet|<1.5. The
             results are compared with several theoretical
             predictions.},
   Doi = {10.1103/physrevlett.111.042003},
   Key = {fds307594}
}

@article{fds356747,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
             M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Measurement of the cross section for inclusive
             isolated-photon production in pp collisions at s=13 TeV
             using the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {770},
   Pages = {473-493},
   Year = {2017},
   Month = {July},
   url = {http://dx.doi.org/10.1016/j.physletb.2017.04.072},
   Abstract = {Inclusive isolated-photon production in pp collisions at a
             centre-of-mass energy of 13 TeV is studied with the ATLAS
             detector at the LHC using a data set with an integrated
             luminosity of 3.2 fb−1. The cross section is measured as a
             function of the photon transverse energy above 125 GeV in
             different regions of photon pseudorapidity.
             Next-to-leading-order perturbative QCD and Monte Carlo
             event-generator predictions are compared to the
             cross-section measurements and provide an adequate
             description of the data.},
   Doi = {10.1016/j.physletb.2017.04.072},
   Key = {fds356747}
}

@article{fds356684,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Measurement of the cross section for isolated-photon plus
             jet production in ppcollisions at √s=13TeV using the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {780},
   Pages = {578-602},
   Year = {2018},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.03.035},
   Abstract = {The dynamics of isolated-photon production in association
             with a jet in proton–proton collisions at a centre-of-mass
             energy of 13 TeV are studied with the ATLAS detector at the
             LHC using a dataset with an integrated luminosity of 3.2
             fb−1. Photons are required to have transverse energies
             above 125 GeV. Jets are identified using the anti-kt
             algorithm with radius parameter R=0.4 and required to have
             transverse momenta above 100 GeV. Measurements of
             isolated-photon plus jet cross sections are presented as
             functions of the leading-photon transverse energy, the
             leading-jet transverse momentum, the azimuthal angular
             separation between the photon and the jet, the photon–jet
             invariant mass and the scattering angle in the photon–jet
             centre-of-mass system. Tree-level plus parton-shower
             predictions from SHERPA and PYTHIA as well as
             next-to-leading-order QCD predictions from JETPHOX and
             SHERPA are compared to the measurements.},
   Doi = {10.1016/j.physletb.2018.03.035},
   Key = {fds356684}
}

@article{fds308131,
   Author = {Acosta, and D, and others},
   Title = {Measurement of the cross section for prompt diphoton
             production in p anti-p collisions at sqrt[s]=1.96
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {95},
   Number = {2},
   Pages = {022003},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/physrevlett.95.022003},
   Abstract = {http://arxiv.org/abs/hep-ex/0412050},
   Doi = {10.1103/physrevlett.95.022003},
   Key = {fds308131}
}

@article{fds307838,
   Author = {Aaltonen, TEA},
   Title = {Measurement of the Cross Section for Prompt Isolated
             Diphoton Production in $p\overline{p}$ Collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {10},
   Pages = {102003},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.102003},
   Abstract = {This Letter reports a measurement of the cross section of
             prompt isolated photon pair production in pp collisions at a
             total energy square root(s)=1.96  TeV using data of
             5.36  fb(-1) integrated luminosity collected with the
             CDF II detector at the Fermilab Tevatron. The measured cross
             section, differential in basic kinematic variables, is
             compared with three perturbative QCD predictions, a leading
             order parton shower calculation and two next-to-leading
             order calculations. The next-to-leading order calculations
             reproduce most aspects of the data. By including photon
             radiation from quarks before and after hard scattering, the
             parton shower prediction becomes competitive with the
             next-to-leading order predictions.},
   Doi = {10.1103/PhysRevLett.107.102003},
   Key = {fds307838}
}

@article{fds307612,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and d'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
             JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
             M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
             G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
             A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov,
             A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
             N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Riddick, T and Rimondi,
             F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani,
             M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu,
             V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song,
             H and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of the cross section for prompt isolated
             diphoton production using the full CDF run II data
             sample.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {10},
   Pages = {101801},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.110.101801},
   Abstract = {This Letter reports a measurement of the cross section for
             producing pairs of central prompt isolated photons in
             proton-antiproton collisions at a total energy sqrt[s] =
             1.96 TeV using data corresponding to 9.5 fb(-1) integrated
             luminosity collected with the CDF II detector at the
             Fermilab Tevatron. The measured differential cross section
             is compared to three calculations derived from the theory of
             strong interactions. These include a prediction based on a
             leading order matrix element calculation merged with a
             parton shower model, a next-to-leading order calculation,
             and a next-to-next-to-leading order calculation. The first
             and last calculations reproduce most aspects of the data,
             thus showing the importance of higher-order contributions
             for understanding the theory of strong interaction and
             improving measurements of the Higgs boson and searches for
             new phenomena in diphoton final states.},
   Doi = {10.1103/physrevlett.110.101801},
   Key = {fds307612}
}

@article{fds308153,
   Author = {Acosta, and D, and others},
   Title = {Measurement of the cross section for t anti-t production in
             p anti-p collisions using the kinematics of lepton + jets
             events},
   Journal = {Phys. Rev.},
   Volume = {D72},
   Number = {5},
   Pages = {052003},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.72.052003},
   Abstract = {http://arxiv.org/abs/hep-ex/0504053},
   Doi = {10.1103/PhysRevD.72.052003},
   Key = {fds308153}
}

@article{fds307756,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the cross section for the production of a W
             boson in association with b-jets in pp collisions at √s =
             7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {707},
   Number = {5},
   Pages = {418-437},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.12.046},
   Abstract = {A measurement is presented of the cross section for the
             production of a W boson with one or two jets, of which at
             least one must be a b-jet, in pp collisions at √s = 7 TeV.
             Production via top decay is not included in the signal
             definition. The measurement is based on 35 pb-1 of data
             collected with the ATLAS detector at the LHC. The W + b-jet
             cross section is defined for jets reconstructed with the
             antikt clustering algorithm with transverse momentum above
             25 GeV and rapidity within ±2.1. The b-jets are identified
             by reconstructing secondary vertices. The fiducial cross
             section is measured both for the electron and muon decay
             channel of the W boson and is found to be 10.2 ± 1.9(stat)
             ± 2.6(syst) pb for one lepton flavour. The results are
             compared with next-to-leading order QCD calculations, which
             predict a cross section smaller than, though consistent
             with, the measured value.},
   Doi = {10.1016/j.physletb.2011.12.046},
   Key = {fds307756}
}

@article{fds307733,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the cross section for top-quark pair
             production in pp collisions at √s = 7 TeV with the ATLAS
             detector using final states with two high-pT
             leptons},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP05(2012)059},
   Abstract = {A measurement is reported of the production cross section of
             top-quark pairs (tt̄) in proton-proton collisions at a
             center-of-mass energy of 7 TeV recorded with the ATLAS
             detector at the LHC. Candidate events have a signature
             consistent with containing two isolated leptons, large
             missing transverse momentum, and at least two jets. Using a
             data sample corresponding to an integrated luminosity of
             0.70 fb-1, a tt̄ production cross section σtt̄ = 176 ±
             5(stat.)-1111+(syst.) ± 8(lum.) pb is measured for an
             assumed top-quark mass of mt = 172.5 GeV. This measurement
             is in good agreement with Standard Model predictions. ©
             CERN.},
   Doi = {10.1007/JHEP05(2012)059},
   Key = {fds307733}
}

@article{fds336988,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov,
             A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
   Title = {Measurement of the cross section for W-boson production in
             association with jets in pp̄ collisions at
             s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {77},
   Number = {1},
   Year = {2008},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.011108},
   Abstract = {We present a measurement of the cross section for W-boson
             production in association with jets in pp̄ collisions at
             s=1.96TeV. The analysis uses a data sample corresponding to
             an integrated luminosity of 320pb-1 collected with the CDF
             II detector. W bosons are identified in their electron decay
             channel and jets are reconstructed using a cone algorithm.
             For each W+≥n-jet sample (n=1-4) we measure the
             differential cross section dσ(pp̄→W+≥
             n-jet)/dETnth-jet×B(W→eν) with respect to the transverse
             energy ET of the nth-highest ET jet above 20GeV, and the
             total cross section σ(pp̄→W+≥n-jet;ETnth-jet>25GeV)×B(W→eν),
             for a restricted W→eν decay phase space. The cross
             sections, corrected for all detector effects, can be
             directly compared to particle level W+jet(s) predictions. We
             present here comparisons to leading order and
             next-to-leading order predictions. © 2008 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.77.011108},
   Key = {fds336988}
}

@article{fds317303,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurement of the cross section of high transverse momentum
             Z→bb¯ production in proton–proton collisions at √s=8
             TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {738},
   Pages = {25-43},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {November},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.09.020},
   Abstract = {This Letter reports the observation of a high transverse
             momentum Z→bb¯ signal in proton–proton collisions at
             s=8 TeV and the measurement of its production cross section.
             The data analysed were collected in 2012 with the ATLAS
             detector at the LHC and correspond to an integrated
             luminosity of 19.5 fb−1. The Z→bb¯ decay is
             reconstructed from a pair of b-tagged jets, clustered with
             the anti-kt jet algorithm with R=0.4, that have low angular
             separation and form a dijet with pT>200 GeV. The signal
             yield is extracted from a fit to the dijet invariant mass
             distribution, with the dominant, multi-jet background mass
             shape estimated by employing a fully data-driven technique
             that reduces the dependence of the analysis on simulation.
             The fiducial cross section is determined to be
             σZ→bb¯fid=2.02±0.20 (stat.) ±0.25 (syst.)±0.06
             (lumi.) pb=2.02 ±0.33 pb, in good agreement with
             next-to-leading-order theoretical predictions.},
   Doi = {10.1016/j.physletb.2014.09.020},
   Key = {fds317303}
}

@article{fds356579,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
             L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
             JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson,
             TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
             JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
             VA},
   Title = {Measurement of the cross-section and charge asymmetry of W
             bosons produced in proton–proton collisions at √s=8TeV
             with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {9},
   Year = {2019},
   Month = {September},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7199-0},
   Abstract = {This paper presents measurements of the W+→ μ+ν and
             W-→ μ-ν cross-sections and the associated charge
             asymmetry as a function of the absolute pseudorapidity of
             the decay muon. The data were collected in proton–proton
             collisions at a centre-of-mass energy of 8 TeV with the
             ATLAS experiment at the LHC and correspond to a total
             integrated luminosity of 20.2fb-1. The precision of the
             cross-section measurements varies between 0.8 and 1.5% as a
             function of the pseudorapidity, excluding the 1.9%
             uncertainty on the integrated luminosity. The charge
             asymmetry is measured with an uncertainty between 0.002 and
             0.003. The results are compared with predictions based on
             next-to-next-to-leading-order calculations with various
             parton distribution functions and have the sensitivity to
             discriminate between them.},
   Doi = {10.1140/epjc/s10052-019-7199-0},
   Key = {fds356579}
}

@article{fds307752,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the cross-section for b-jets produced in
             association with a Z boson at s=7 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {706},
   Number = {4-5},
   Pages = {295-313},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.11.059},
   Abstract = {A measurement is presented of the inclusive cross-section
             for b-jet production in association with a Z boson in pp
             collisions at a centre-of-mass energy of s=7 TeV. The
             analysis uses the data sample collected by the ATLAS
             experiment in 2010, corresponding to an integrated
             luminosity of approximately 36 pb-1. The event selection
             requires a Z boson decaying into high pT electrons or muons,
             and at least one b-jet, identified by its displaced vertex,
             with transverse momentum pT>25 GeV and rapidity |y|<2.1.
             After subtraction of background processes, the yield is
             extracted from the vertex mass distribution of the candidate
             b-jets. The ratio of this cross-section to the inclusive Z
             cross-section (the average number of b-jets per Z event) is
             also measured. Both results are found to be in good
             agreement with perturbative QCD predictions at
             next-to-leading order. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.11.059},
   Key = {fds307752}
}

@article{fds356711,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Measurement of the cross-section for electroweak production
             of dijets in association with a Z boson in pp collisions at
             s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {775},
   Pages = {206-228},
   Year = {2017},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2017.10.040},
   Abstract = {The cross-section for the production of two jets in
             association with a leptonically decaying Z boson (Zjj) is
             measured in proton–proton collisions at a centre-of-mass
             energy of 13 TeV, using data recorded with the ATLAS
             detector at the Large Hadron Collider, corresponding to an
             integrated luminosity of 3.2 fb−1. The electroweak Zjj
             cross-section is extracted in a fiducial region chosen to
             enhance the electroweak contribution relative to the
             dominant Drell–Yan Zjj process, which is constrained using
             a data-driven approach. The measured fiducial electroweak
             cross-section is σEWZjj = 119±16(stat.)±20(syst.)±2(lumi.)
             fb for dijet invariant mass greater than 250 GeV, and
             34.2±5.8(stat.)±5.5(syst.)±0.7(lumi.) fb for dijet
             invariant mass greater than 1 TeV. Standard Model
             predictions are in agreement with the measurements. The
             inclusive Zjj cross-section is also measured in six
             different fiducial regions with varying contributions from
             electroweak and Drell–Yan Zjj production.},
   Doi = {10.1016/j.physletb.2017.10.040},
   Key = {fds356711}
}

@article{fds356703,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Measurement of the cross-section for producing a W boson in
             association with a single top quark in pp collisions at
             √s=13 TeV with ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {1},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2018)063},
   Abstract = {The inclusive cross-section for the associated production of
             a W boson and top quark is measured using data from
             proton-proton collisions at s=13 TeV. The dataset
             corresponds to an integrated luminosity of 3.2 fb−1, and
             was collected in 2015 by the ATLAS detector at the Large
             Hadron Collider at CERN. Events are selected requiring two
             opposite sign isolated leptons and at least one jet; they
             are separated into signal and control regions based on their
             jet multiplicity and the number of jets that are identified
             as containing b hadrons. The W t signal is then separated
             from the tt¯ background using boosted decision tree
             discriminants in two regions. The cross-section is extracted
             by fitting templates to the data distributions, and is
             measured to be σW t = 94 ± 10(stat.)− 22+ 28(syst.) ±
             2(lumi.) pb. The measured value is in good agreement with
             the SM prediction of σtheory = 71.7±1.8 (scale)± 3.4
             (PDF) pb [1].[Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP01(2018)063},
   Key = {fds356703}
}

@article{fds310343,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov,
             VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurement of the cross-section of high transverse momentum
             vector bosons reconstructed as single jets and studies of
             jet substructure in pp collisions at √s = 7 TeV with the
             ATLAS detector},
   Journal = {New Journal of Physics},
   Volume = {16},
   Number = {11},
   Pages = {113013-113013},
   Publisher = {IOP Publishing},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1088/1367-2630/16/11/113013},
   Abstract = {This paper presents a measurement of the cross-section for
             high transverse momentum W and Z bosons produced in pp
             collisions and decaying to all-hadronic final states. The
             data used in the analysis were recorded by the ATLAS
             detector at the CERN Large Hadron Collider at a
             centre-of-mass energy of and correspond to an integrated
             luminosity of . The measurement is performed by
             reconstructing the boosted W or Z bosons in single jets. The
             reconstructed jet mass is used to identify the W and Z
             bosons, and a jet substructure method based on energy
             cluster information in the jet centre-of-mass frame is used
             to suppress the large multi-jet background. The
             cross-section for events with a hadronically decaying W or Z
             boson, with transverse momentum and pseudorapidity , is
             measured to be pb and is compared to next-to-leading-order
             calculations. The selected events are further used to study
             jet grooming techniques.},
   Doi = {10.1088/1367-2630/16/11/113013},
   Key = {fds310343}
}

@article{fds374210,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
             J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
             GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
             Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
             C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
             M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
             SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
   Title = {Measurement of the cross-sections of the electroweak and
             total production of a Zγ pair in association with two jets
             in pp collisions at s=13 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {846},
   Year = {2023},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.138222},
   Abstract = {This Letter presents the measurement of the fiducial and
             differential cross-sections of the electroweak production of
             a Zγ pair in association with two jets. The analysis uses
             140 fb−1 of LHC proton–proton collision data taken at
             s=13 TeV recorded by the ATLAS detector during the years
             2015–2018. Events with a Z boson candidate decaying into
             either an e+e− or μ+μ− pair, a photon and two jets are
             selected. The electroweak component is extracted by
             requiring a large dijet invariant mass and by using the
             information about the centrality of the system and is
             measured with an observed and expected significance well
             above five standard deviations. The fiducial pp→Zγjj
             cross-section for the electroweak production is measured to
             be 3.6 ± 0.5 fb. The total fiducial cross-section that also
             includes contributions where the jets arise from strong
             interactions is measured to be 16.8−1.8+2.0 fb. The
             results are consistent with the Standard Model predictions.
             Differential cross-sections are also measured using the same
             events and are compared with parton-shower Monte Carlo
             simulations. Good agreement is observed between data and
             predictions.},
   Doi = {10.1016/j.physletb.2023.138222},
   Key = {fds374210}
}

@article{fds356753,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Erbacher, R and Errede, S and Esham,
             B},
   Title = {Measurement of the D+ -meson production cross section at low
             transverse momentum in pp¯ collisions at s=1.96
             TeV},
   Journal = {Physical Review D},
   Volume = {95},
   Number = {9},
   Year = {2017},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.95.092006},
   Abstract = {We report on a measurement of the D+-meson production cross
             section as a function of transverse momentum (pT) in
             proton-antiproton (pp) collisions at 1.96 TeV center-of-mass
             energy, using the full data set collected by the Collider
             Detector at Fermilab in Tevatron Run II and corresponding to
             10 fb-1 of integrated luminosity. We use D+→K-π+π+
             decays fully reconstructed in the central rapidity region
             |y|<1 with transverse momentum down to 1.5 GeV/c, a range
             previously unexplored in pp collisions. Inelastic
             pp-scattering events are selected online using minimally
             biasing requirements followed by an optimized offline
             selection. The K-π+π+ mass distribution is used to
             identify the D+ signal, and the D+ transverse
             impact-parameter distribution is used to separate prompt
             production, occurring directly in the hard-scattering
             process, from secondary production from b-hadron decays. We
             obtain a prompt D+ signal of 2950 candidates corresponding
             to a total cross section σ(D+,1.5<pT<14.5
             GeV/c,|y|<1)=71.9±6.8(stat)±9.3(syst) μb. While the
             measured cross sections are consistent with theoretical
             estimates in each pT bin, the shape of the observed pT
             spectrum is softer than the expectation from quantum
             chromodynamics. The results are unique in pp collisions and
             can improve the shape and uncertainties of future
             predictions.},
   Doi = {10.1103/PhysRevD.95.092006},
   Key = {fds356753}
}

@article{fds356771,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of the dependence of transverse energy
             production at large pseudorapidity on the hard-scattering
             kinematics of proton–proton collisions at √s=2.76 TeV
             with ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {756},
   Pages = {10-28},
   Year = {2016},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.02.056},
   Abstract = {The relationship between jet production in the central
             region and the underlying-event activity in a
             pseudorapidity-separated region is studied in 4.0 pb−1 of
             s=2.76 TeV pp collision data recorded with the ATLAS
             detector at the LHC. The underlying event is characterised
             through measurements of the average value of the sum of the
             transverse energy at large pseudorapidity downstream of one
             of the protons, which are reported here as a function of
             hard-scattering kinematic variables. The hard scattering is
             characterised by the average transverse momentum and
             pseudorapidity of the two highest transverse momentum jets
             in the event. The dijet kinematics are used to estimate, on
             an event-by-event basis, the scaled longitudinal momenta of
             the hard-scattered partons in the target and projectile
             beam-protons moving toward and away from the region
             measuring transverse energy, respectively. Transverse energy
             production at large pseudorapidity is observed to decrease
             with a linear dependence on the longitudinal momentum
             fraction in the target proton and to depend only weakly on
             that in the projectile proton. The results are compared to
             the predictions of various Monte Carlo event generators,
             which qualitatively reproduce the trends observed in data
             but generally underpredict the overall level of transverse
             energy at forward pseudorapidity.},
   Doi = {10.1016/j.physletb.2016.02.056},
   Key = {fds356771}
}

@article{fds307812,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of the difference in CP-violating asymmetries in
             D(0)→K(+)K(-) and D(0)→π(+)π(-) decays at
             CDF.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {11},
   Pages = {111801},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevlett.109.111801},
   Abstract = {We report a measurement of the difference (ΔA(CP)) between
             time-integrated CP-violating asymmetries in D(0)→K(+)K(-)
             and D(0)→π(+)π(-) decays reconstructed in the full data
             set of proton-antiproton collisions collected by the
             Collider Detector at Fermilab, corresponding to
             9.7  fb(-1) of integrated luminosity. The strong decay
             D(*+)→D(0)π(+) is used to identify the charm meson at
             production as D(0) or D[over ¯](0). We measure
             ΔA(CP)=[-0.62±0.21(stat)±0.10(syst)]%, which differs from
             zero by 2.7 Gaussian standard deviations. This result
             supports similar evidence for CP violation in charm-quark
             decays obtained in proton-proton collisions.},
   Doi = {10.1103/physrevlett.109.111801},
   Key = {fds307812}
}

@article{fds307596,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
             JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
             A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
             C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
             L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Measurement of the differential cross section
             dσ/d(cosθ(t)) for Top-Quark Pair Production in pp
             Collisions at sqrt[s] = 1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {18},
   Pages = {182002},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.111.182002},
   Abstract = {We report a measurement of the differential cross section
             dσ/d(cosθ(t)) for top-quark pair production as a function
             of the top-quark production angle in proton-antiproton
             collisions at sqrt[s] = 1.96 TeV. This measurement is
             performed using data collected with the CDF II detector at
             the Tevatron, corresponding to an integrated luminosity of
             9.4 fb(-1). We employ the Legendre polynomials to
             characterize the shape of the differential cross section at
             the parton level. The observed Legendre coefficients are in
             good agreement with the prediction of the
             next-to-leading-order standard-model calculation, with the
             exception of an excess linear-term coefficient a(1) = 0.40
             ± 0.12, compared to the standard-model prediction of
             a(1)=0.15(-0.03)(+0.07).},
   Doi = {10.1103/physrevlett.111.182002},
   Key = {fds307596}
}

@article{fds356635,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Measurement of the differential cross sections for W -boson
             production in association with jets in p p collisions at s
             =1.96 TeV MEASUREMENT of the DIFFERENTIAL CROSS ⋯ T.
             AALTONEN et al.},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {11},
   Year = {2018},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.112005},
   Abstract = {This paper presents a study of the production of a single W
             boson in association with one or more jets in
             proton-antiproton collisions at s=1.96 TeV, using the entire
             data set collected in 2001-2011 by the Collider Detector at
             Fermilab at the Tevatron, which corresponds to an integrated
             luminosity of 9.0 fb-1. The W boson is identified through
             its leptonic decays into electron and muon. The production
             cross sections are measured for each leptonic decay mode and
             combined after testing that the ratio of the W(→μν)+jets
             cross section to the W(→eν)+jets cross section agrees
             with the hypothesis of e-μ lepton universality. The
             combination of measured cross sections, differential in the
             inclusive jet multiplicity (W+≥N jets with N=1, 2, 3, or
             4) and in the transverse energy of the leading jet, are
             compared with theoretical predictions.},
   Doi = {10.1103/PhysRevD.98.112005},
   Key = {fds356635}
}

@article{fds307570,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Measurement of the differential cross-section of B+ meson
             production in pp collisions at √s = 7 TeV at
             ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {10},
   Pages = {1-37},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP10(2013)042},
   Abstract = {The production cross-section of B+ mesons is measured as a
             function of transverse momentum pT and rapidity y in
             proton-proton collisions at centre-of-mass energy √s = 7
             TeV, using 2.4 fb-1 of data recorded with the ATLAS detector
             at the Large Hadron Collider. The differential production
             cross-sections, determined in the range 9 GeV < pT < 120 GeV
             and |y| < 2:25, are compared to next-to-leading-order
             theoretical predictions. Copyright CERN.},
   Doi = {10.1007/JHEP10(2013)042},
   Key = {fds307570}
}

@article{fds356780,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Measurement of the differential cross-section of highly
             boosted top quarks as a function of their transverse
             momentum in s =8 TeV proton-proton collisions using the
             ATLAS detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {3},
   Year = {2016},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.032009},
   Abstract = {The differential cross-section for pair production of top
             quarks with high transverse momentum is measured in 20.3
             fb-1 of proton-proton collisions at a center-of-mass energy
             of 8 TeV. The measurement is performed for tt¯ events in
             the lepton+jets channel. The cross-section is reported as a
             function of the hadronically decaying top quark transverse
             momentum for values above 300 GeV. The hadronically decaying
             top quark is reconstructed as an anti-kt jet with radius
             parameter R=1.0 and identified with jet substructure
             techniques. The observed yield is corrected for detector
             effects to obtain a cross-section at particle level in a
             fiducial region close to the event selection. A parton-level
             cross-section extrapolated to the full phase space is also
             reported for top quarks with transverse momentum above 300
             GeV. The predictions of a majority of next-to-leading-order
             and leading-order matrix-element Monte Carlo generators are
             found to agree with the measured cross-sections.},
   Doi = {10.1103/PhysRevD.93.032009},
   Key = {fds356780}
}

@article{fds323671,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
             A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
             J},
   Title = {Measurement of the differential cross-sections of prompt and
             non-prompt production of [Formula: see text] and [Formula:
             see text] in pp collisions at [Formula: see text] and
             8 TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {283},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4050-8},
   Abstract = {The production rates of prompt and non-prompt [Formula: see
             text] and [Formula: see text] mesons in their dimuon decay
             modes are measured using 2.1 and 11.4 fb[Formula: see text]
             of data collected with the ATLAS experiment at the Large
             Hadron Collider, in proton-proton collisions at [Formula:
             see text] and 8 respectively. Production cross-sections for
             prompt as well as non-prompt sources, ratios of [Formula:
             see text] to [Formula: see text] production, and the
             fractions of non-prompt production for [Formula: see text]
             and [Formula: see text] are measured as a function of meson
             transverse momentum and rapidity. The measurements are
             compared to theoretical predictions.},
   Doi = {10.1140/epjc/s10052-016-4050-8},
   Key = {fds323671}
}

@article{fds308100,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the dipion mass spectrum in X(3872) --> J/psi
             pi+ pi- decays},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {10},
   Pages = {102002},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.102002},
   Abstract = {We measure the dipion mass spectrum in X(3872) --> J/psi
             pi++ pi+- decays using 360 pb-1 of p anti-p collisions at
             s**(1/2) = 1.96 TeV collected with the CDF II detector. The
             spectrum is fit with predictions for odd C-parity (3S_1,
             1P_1, and 3D_J) charmonia decaying to J/psi pi++ pi+-, as
             well as even C-parity states in which the pi+ons are from
             rho0 decay. The latter case also encompasses exotic
             interpretations, such as D0 D-bar*0 molecule. Only the 3S_1
             and J/psi rho hypotheses are compatible with our data. Since
             3S_1 is untenable on other grounds, decay via J/psi rho is
             favored, which implies C = +1 for the X(3872). Models for
             different J/psi-rho angular momenta L are considered.
             Flexibility in the models, especially the introduction of
             rho-omega interference, enable good descriptions of our data
             for both L = 0 and 1.},
   Doi = {10.1103/physrevlett.96.102002},
   Key = {fds308100}
}

@article{fds307564,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Measurement of the distributions of event-by-event flow
             harmonics in lead-lead collisions at √SNN =
             2.76 TeV with the ATLAS detector at the LHC},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2013)183},
   Abstract = {The distributions of event-by-event harmonic flow
             coefficients υn for n = 2-4 are measured in √sNN =
             2.76TeV Pb+Pb collisions using the ATLAS detector at the
             LHC. The measurements are performed using charged particles
             with transverse momentum pT > 0.5GeV and in the
             pseudorapidity range |η| < 2.5 in a dataset of
             approximately 7 μb-1 recorded in 2010. The shapes of the
             υn distributions suggest that the associated flow vectors
             are described by a two-dimensional Gaussian function in
             central collisions for υ2 and over most of the measured
             centrality range for υ3 and υ4. Significant deviations
             from this function are observed for υ2 in mid-central and
             peripheral collisions, and a small deviation is observed for
             υ3 in mid-central collisions. In order to be sensitive to
             these deviations, it is shown that the commonly used
             multi-particle cumulants, involving four particles or more,
             need to be measured with a precision better than a few
             percent. The υn distributions are also measured
             independently for charged particles with 0.5 < pT < 1 GeV
             and pT > 1 GeV. When these distributions are rescaled to the
             same mean values, the adjusted shapes are found to be nearly
             the same for these two pT ranges. The υn distributions are
             compared with the eccentricity distributions from two models
             for the initial collision geometry: a Glauber model and a
             model that includes corrections to the initial geometry due
             to gluon saturation effects. Both models fail to describe
             the experimental data consistently over most of the measured
             centrality range. Copyright CERN.},
   Doi = {10.1007/JHEP11(2013)183},
   Key = {fds307564}
}

@article{fds321104,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Measurement of the double-differential high-mass Drell-Yan
             cross section in pp collisions at √s = 8 TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2016)009},
   Abstract = {This paper presents a measurement of the double-differential
             cross section for the Drell-Yan Z/γ∗ → ℓ+ℓ− and
             photon-induced γγ → ℓ+ℓ− processes where ℓ is an
             electron or muon. The measurement is performed for invariant
             masses of the lepton pairs, mℓℓ, between 116 GeV and
             1500 GeV using a sample of 20.3 fb−1 of pp collisions data
             at centre-of-mass energy of s=8 TeV collected by the ATLAS
             detector at the LHC in 2012. The data are presented double
             differentially in invariant mass and absolute dilepton
             rapidity as well as in invariant mass and absolute
             pseudorapidity separation of the lepton pair. The
             single-differential cross section as a function of mℓℓ
             is also reported. The electron and muon channel measurements
             are combined and a total experimental precision of better
             than 1% is achieved at low mℓℓ. A comparison to
             next-to-next-to-leading order perturbative QCD predictions
             using several recent parton distribution functions and
             including next-to-leading order electroweak effects
             indicates the potential of the data to constrain parton
             distribution functions. In particular, a large impact of the
             data on the photon PDF is demonstrated.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP08(2016)009},
   Key = {fds321104}
}

@article{fds356717,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Measurement of the Drell-Yan triple-differential cross
             section in pp collisions at √s=8 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {12},
   Year = {2017},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2017)059},
   Abstract = {This paper presents a measurement of the triple-differential
             cross section for the Drell-Yan process Z/γ* → ℓ+ℓ−
             where ℓ is an electron or a muon. The measurement is
             performed for invariant masses of the lepton pairs, mℓℓ,
             between 46 and 200 GeV using a sample of 20.2 fb−1 of pp
             collisions data at a centre-of-mass energy of s=8 TeV
             collected by the ATLAS detector at the LHC in 2012. The data
             are presented in bins of invariant mass, absolute dilepton
             rapidity, |yℓℓ|, and the angular variable cos θ*
             between the outgoing lepton and the incoming quark in the
             Collins-Soper frame. The measurements are performed in the
             range |yℓℓ| < 2.4 in the muon channel, and extended to
             |yℓℓ| < 3.6 in the electron channel. The cross sections
             are used to determine the Z boson forward-backward asymmetry
             as a function of |yℓℓ| and mℓℓ. The measurements
             achieve high-precision, below the percent level in the pole
             region, excluding the uncertainty in the integrated
             luminosity, and are in agreement with predictions. These
             precision data are sensitive to the parton distribution
             functions and the effective weak mixing angle.},
   Doi = {10.1007/JHEP12(2017)059},
   Key = {fds356717}
}

@article{fds307545,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov,
             VV and Dos Santos and SPA and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V},
   Title = {Measurement of the electroweak production of dijets in
             association with a Z-boson and distributions sensitive to
             vector boson fusion in proton-proton collisions at √s= 8
             TeV using the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {4},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP04(2014)031},
   Doi = {10.1007/JHEP04(2014)031},
   Key = {fds307545}
}

@article{fds363186,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
             SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury,
             KA and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari,
             N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C},
   Title = {Measurement of the energy asymmetry in tt¯ j production at
             13 TeV with the ATLAS experiment and interpretation in the
             SMEFT framework},
   Journal = {European Physical Journal C},
   Volume = {82},
   Number = {4},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2022},
   Month = {April},
   url = {http://dx.doi.org/10.1140/epjc/s10052-022-10101-w},
   Abstract = {A measurement of the energy asymmetry in jet-associated
             top-quark pair production is presented using 139fb-1 of data
             collected by the ATLAS detector at the Large Hadron Collider
             during pp collisions at s=13TeV. The observable measures the
             different probability of top and antitop quarks to have the
             higher energy as a function of the jet scattering angle with
             respect to the beam axis. The energy asymmetry is measured
             in the semileptonic tt¯ decay channel, and the hadronically
             decaying top quark must have transverse momentum above
             350GeV. The results are corrected for detector effects to
             particle level in three bins of the scattering angle of the
             associated jet. The measurement agrees with the SM
             prediction at next-to-leading-order accuracy in quantum
             chromodynamics in all three bins. In the bin with the
             largest expected asymmetry, where the jet is emitted
             perpendicular to the beam, the energy asymmetry is measured
             to be - 0.043 ± 0.020 , in agreement with the SM prediction
             of - 0.037 ± 0.003. Interpreting this result in the
             framework of the Standard Model effective field theory
             (SMEFT), it is shown that the energy asymmetry is sensitive
             to the top-quark chirality in four-quark operators and is
             therefore a valuable new observable in global SMEFT
             fits.},
   Doi = {10.1140/epjc/s10052-022-10101-w},
   Key = {fds363186}
}

@article{fds362727,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
             SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury,
             KA and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
   Title = {Measurement of the energy response of the ATLAS calorimeter
             to charged pions from W±→ τ±(→
             π±ντ) ντ events in
             Run 2 data},
   Journal = {European Physical Journal C},
   Volume = {82},
   Number = {3},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2022},
   Month = {March},
   url = {http://dx.doi.org/10.1140/epjc/s10052-022-10117-2},
   Abstract = {The energy response of the ATLAS calorimeter is measured for
             single charged pions with transverse momentum in the range
             10 < pT< 300 GeV. The measurement is performed using 139 fb
             - 1 of LHC proton–proton collision data at s=13 TeV taken
             in Run 2 by the ATLAS detector. Charged pions originating
             from τ-lepton decays are used to provide a sample of
             high-pT isolated particles, where the composition is known,
             to test an energy regime that has not previously been probed
             by in situ single-particle measurements. The calorimeter
             response to single-pions is observed to be overestimated by
             ∼ 2 % across a large part of the pT spectrum in the
             central region and underestimated by ∼ 4 % in the endcaps
             in the ATLAS simulation. The uncertainties in the
             measurements are ≲ 1 % for 15 < pT< 185 GeV in the central
             region. To investigate the source of the discrepancies, the
             width of the distribution of the ratio of calorimeter energy
             to track momentum, the energies per layer and response in
             the hadronic calorimeter are also compared between data and
             simulation.},
   Doi = {10.1140/epjc/s10052-022-10117-2},
   Key = {fds362727}
}

@article{fds356698,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Measurement of the exclusive γγ → μ+μ
             process in proton–proton collisions at √s=13TeV with the
             ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {777},
   Pages = {303-323},
   Year = {2018},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2017.12.043},
   Abstract = {The production of exclusive γγ→μ+μ− events in
             proton–proton collisions at a centre-of-mass energy of 13
             TeV is measured with the ATLAS detector at the LHC, using
             data corresponding to an integrated luminosity of 3.2
             fb−1. The measurement is performed for a dimuon invariant
             mass of 12GeV<mμ+μ−<70GeV. The integrated cross-section
             is determined within a fiducial acceptance region of the
             ATLAS detector and differential cross-sections are measured
             as a function of the dimuon invariant mass. The results are
             compared to theoretical predictions both with and without
             corrections for absorptive effects.},
   Doi = {10.1016/j.physletb.2017.12.043},
   Key = {fds356698}
}

@article{fds307631,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim, A and Amram,
             N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M},
   Title = {Measurement of the flavour composition of dijet events in pp
             collisions at √s = 7 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {73},
   Number = {2},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2301-5},
   Abstract = {This paper describes a measurement of the flavour
             composition of dijet events produced in pp collisions at
             √s = 7 TeV using the ATLAS detector. The measurement uses
             the full 2010 data sample, corresponding to an integrated
             luminosity of 39 pb<sup>−1</sup>. Six possible
             combinations of light, charm and bottom jets are identified
             in the dijet events, where the jet flavour is defined by the
             presence of bottom, charm or solely light flavour hadrons in
             the jet. Kinematic variables, based on the properties of
             displaced decay vertices and optimised for jet flavour
             identification, are used in a multidimensional template fit
             to measure the fractions of these dijet flavour states as
             functions of the leading jet transverse momentum in the
             range 40 GeV to 500 GeV and jet rapidity |y| < 2.1. The fit
             results agree with the predictions of leading- and
             next-to-leading-order calculations, with the exception of
             the dijet fraction composed of bottom and light flavour
             jets, which is underestimated by all models at large
             transverse jet momenta. The ability to identify jets
             containing two b-hadrons, originating from e.g. gluon
             splitting, is demonstrated. The difference between bottom
             jet production rates in leading and subleading jets is
             consistent with the next-to-leading-order
             predictions.},
   Doi = {10.1140/epjc/s10052-013-2301-5},
   Key = {fds307631}
}

@article{fds321120,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Erbacher, R and Errede, S and Esham,
             B},
   Title = {Measurement of the forward-backward asymmetry in low-mass
             bottom-quark pairs produced in proton-antiproton
             collisions},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.112003},
   Abstract = {We report a measurement of the forward-backward asymmetry,
             AFB, in bb pairs produced in proton-antiproton collisions
             and identified by muons from semileptonic b-hadron decays.
             The event sample is collected at a center-of-mass energy of
             s=1.96 TeV with the CDF II detector and corresponds to 6.9
             fb-1 of integrated luminosity. We obtain an integrated
             asymmetry of AFB(bb)=(1.2±0.7)% at the particle level for
             b-quark pairs with invariant mass, mbb, down to 40 GeV/c2
             and measure the dependence of AFB(bb) on mbb. The results
             are compatible with expectations from the standard
             model.},
   Doi = {10.1103/PhysRevD.93.112003},
   Key = {fds321120}
}

@article{fds307873,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of the Forward-Backward Asymmetry in the
             ${B}\rightarrow{K}^{(*)}\mu^{+}\mu^{-}$ Decay and First
             Observation of the ${B}_{s}^{0}$\rightarrow${}$\phi${}{$\mu${}}^{+}{$\mu${}}^{-}$
             Decay},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {16},
   Pages = {161801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.161801},
   Abstract = {We reconstruct the rare decays B(+)→K(+)μ(+0μ(-0,
             B90)→K*(892)(0)μ(+)μ(-), and B(s)(0)→ϕ(1020)μ(+)μ(-)
             in a data sample corresponding to 4.4  fb(-1) collected
             in pp collisions at √[s]=1.96  TeV by the CDF II
             detector at the Tevatron Collider. Using 121±16
             B(+)→K(+)μ(+)μ(-) and 101±12 B(0)→K(*0)μ(+)μ(-)
             decays we report the branching ratios. In addition, we
             report the differential branching ratio and the muon
             forward-backward asymmetry in the B(+) and B(0) decay modes,
             and the K(*0) longitudinal polarization fraction in the B(0)
             decay mode with respect to the squared dimuon mass. These
             are consistent with the predictions, and most recent
             determinations from other experiments and of comparable
             accuracy. We also report the first observation of the
             B(s)(0)→ϕμ(+)μ(-) decay and measure its branching ratio
             BR(B(s)(0)→ϕμ(+)μ(-))=[1.44±0.33±0.46]×10(-6) using
             27±6 signal events. This is currently the most rare B(s)(0)
             decay observed.},
   Doi = {10.1103/PhysRevLett.106.161801},
   Key = {fds307873}
}

@article{fds313597,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the forward-backward asymmetry of electron
             and muon pair-production in pp collisions at √s=7 TeV with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {9},
   Pages = {1-43},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2015)049},
   Abstract = {This paper presents measurements from the ATLAS experiment
             of the forward-backward asymmetry in the reaction pp →
             Z/γ* → l+l−, with l being electrons or muons, and the
             extraction of the effective weak mixing angle. The results
             are based on the full set of data collected in 2011 in pp
             collisions at the LHC at (Formula presented.), corresponding
             to an integrated luminosity of 4.8 fb−1. The measured
             asymmetry values are found to be in agreement with the
             corresponding Standard Model predictions. The combination of
             the muon and electron channels yields a value of the
             effective weak mixing angle of sin2θefflept = 0.2308 ±
             0.0005(stat.) ± 0.0006(syst.) ± 0.0009(PDF), where the
             first uncertainty corresponds to data statistics, the second
             to systematic effects and the third to knowledge of the
             parton density functions. This result agrees with the
             current world average from the Particle Data Group
             fit.},
   Doi = {10.1007/JHEP09(2015)049},
   Key = {fds313597}
}

@article{fds321121,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Erbacher, R and Errede, S and Esham,
             B},
   Title = {Measurement of the forward-backward asymmetry of top-quark
             and antiquark pairs using the full CDF Run II data
             set},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.112005},
   Abstract = {We measure the forward-backward asymmetry of the production
             of top-quark and antiquark pairs in proton-antiproton
             collisions at center-of-mass energy s=1.96 TeV using the
             full data set collected by the Collider Detector at Fermilab
             (CDF) in Tevatron Run II corresponding to an integrated
             luminosity of 9.1 fb-1. The asymmetry is characterized by
             the rapidity difference between top quarks and antiquarks
             (Δy) and measured in the final state with two charged
             leptons (electrons and muons). The inclusive asymmetry,
             corrected to the entire phase space at parton level, is
             measured to be AFBtt=0.12±0.13, consistent with the
             expectations from the standard model (SM) and previous CDF
             results in the final state with a single charged lepton. The
             combination of the CDF measurements of the inclusive AFBtt
             in both final states yields AFBtt=0.160±0.045, which is
             consistent with the SM predictions. We also measure the
             differential asymmetry as a function of Δy. A linear fit to
             AFBtt(|Δy|), assuming zero asymmetry at Δy=0, yields a
             slope of α=0.14±0.15, consistent with the SM prediction
             and the previous CDF determination in the final state with a
             single charged lepton. The combined slope of AFBtt(|Δy|) in
             the two final states is α=0.227±0.057, which is 2.0σ
             larger than the SM prediction.},
   Doi = {10.1103/PhysRevD.93.112005},
   Key = {fds321121}
}

@article{fds323244,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
             AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
             JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
             D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko,
             I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
             E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
             C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher,
             F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
             D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
             KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
             PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
             BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
             AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
             SW and Lefevre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen,
             D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson,
             M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic,
             N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
             B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
             C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti,
             R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
             C and Pompoš, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy,
             L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard,
             PF},
   Title = {Measurement of the forward-backward charge asymmetry from
             W→ev production in pp̄ collisions at √s=1.96
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {5},
   Pages = {1-9},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.051104},
   Abstract = {We report a measurement of the forward-backward charge
             asymmetry of electrons from W boson decays in pp̄
             collisions at √s=1.96 TeV using a data sample of 170 pb-1
             collected by the Collider Detector at Fermilab. The
             asymmetry is measured as a function of electron rapidity and
             transverse energy and provides new input on the momentum
             fraction dependence of the u and d quark parton distribution
             functions within the proton. © 2005 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.71.051104},
   Key = {fds323244}
}

@article{fds356612,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S},
   Title = {Measurement of the four-lepton invariant mass spectrum in 13
             TeV proton-proton collisions with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {4},
   Year = {2019},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2019)048},
   Abstract = {A measurement of the four-lepton invariant mass spectrum is
             made with the ATLAS detector, using an integrated luminosity
             of 36.1 fb−1 of proton-proton collisions at s = 13 TeV
             delivered by the Large Hadron Collider. The differential
             cross-section is measured for events containing two
             same-flavour opposite-sign lepton pairs. It exhibits a rich
             structure, with different mass regions dominated in the
             Standard Model by single Z boson production, Higgs boson
             production, and Z boson pair production, and non-negligible
             interference effects at high invariant masses. The
             measurement is compared with state-of-the-art Standard Model
             calculations, which are found to be consistent with the
             data. These calculations are used to interpret the data in
             terms of gg → ZZ → 4ℓ and Z → 4ℓ subprocesses, and
             to place constraints on a possible contribution from physics
             beyond the Standard Model.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP04(2019)048},
   Key = {fds356612}
}

@article{fds337969,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
             P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley,
             M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Copic, K and Cordelli, M and Cortiana, G and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson,
             R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and Barbaro,
             PD and Cecco, SD and Deisher, A and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler,
             A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski,
             D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes,
             RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori,
             M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
             JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Koay, SA and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
             M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, RS and Lucchesi, D and Lueck,
             J and Luci, C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou,
             A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pinera, L and Pitts,
             K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn,
             F and Pronko, A and Proudfoot, J and Ptohos, F and Pueschel, E and Punzi,
             G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle,
             T and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
             AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shiraishi,
             S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith,
             JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer, B},
   Title = {Measurement of the fraction of tt̄ production via
             gluon-gluon fusion in pp̄ collisions at
             s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {3},
   Pages = {031101},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.031101},
   Abstract = {We present a measurement of the ratio of the tt̄ production
             cross section via gluon-gluon fusion to the total tt̄
             production cross section in pp̄ collisions at s=1.96TeV at
             the Tevatron. Using a data sample with an integrated
             luminosity of 955pb-1 recorded by the CDF II detector at
             Fermilab, we select events based on the tt̄ decay to
             lepton+jets. Using an artificial neural network technique we
             discriminate between tt̄ events produced via qq̄
             annihilation and gg fusion, and find Gf=σ(gg→tt̄)/
             σ(pp̄→tt̄)&lt;0.33 at the 68% confidence level. This
             result is combined with a previous measurement to obtain the
             most stringent measurement of this quantity by CDF to date,
             Gf=0.07-0.07+0.15. © 2009 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.79.031101},
   Key = {fds337969}
}

@article{fds308077,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the Helicity Fractions of W Bosons from Top
             Quark Decays using Fully Reconstructed \boldmath${t\bar{t}}$
             Events with CDF II},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {5},
   Pages = {052001},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.052001},
   Abstract = {We present a measurement of the fractions F0 and F+ of
             longitudinally polarized and right-handed W bosons in
             top-quark decays using data collected with the CDF II
             detector. The data set used in the analysis corresponds to
             an integrated luminosity of approximately 318 pb-1. We
             select t[overline t] candidate events with one lepton, at
             least four jets, and missing transverse energy. Our helicity
             measurement uses the decay angle theta*, which is defined as
             the angle between the momentum of the charged lepton in the
             W boson rest frame and the W momentum in the top-quark rest
             frame. The costheta* distribution in the data is determined
             by full kinematic reconstruction of the t[overline t]
             candidates. We find F0=0.85-0.22+0.15(stat)$\pm$0.06(syst)
             and F+=0.05-0.05+0.11(stat)$\pm$0.03(syst), which is
             consistent with the standard model prediction. We set an
             upper limit on the fraction of right-handed W bosons of
             F+},
   Doi = {10.1103/PhysRevD.75.052001},
   Key = {fds308077}
}

@article{fds308111,
   Author = {collaboration, CDF},
   Title = {Measurement of the Helicity of W Bosons in Top Quark
             Decays},
   Journal = {Phys.Rev.Lett.},
   Volume = {84},
   Number = {11},
   Pages = {216-221},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.111103},
   Abstract = {http://arXiv.org/ps/hep-ex/9909042},
   Doi = {10.1103/PhysRevD.73.111103},
   Key = {fds308111}
}

@article{fds356693,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Measurement of the Higgs boson coupling properties in the H
             → ZZ  → 4ℓ decay channel at √s=13 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {3},
   Year = {2018},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2018)095},
   Abstract = {The coupling properties of the Higgs boson are studied in
             the four-lepton (e, μ) decay channel using 36.1 fb−1 of
             pp collision data from the LHC at a centre-of-mass energy of
             13 TeV collected by the ATLAS detector. Cross sections are
             measured for the main production modes in several exclusive
             regions of the Higgs boson production phase space and are
             interpreted in terms of coupling modifiers. The inclusive
             cross section times branching ratio for H → ZZ∗ decay
             and for a Higgs boson absolute rapidity below 2.5 is
             measured to be 1. 73− 0.23+ 0.24(stat.)− 0.08+
             0.10(exp.) ± 0.04(th.) pb compared to the Standard Model
             prediction of 1.34±0.09 pb. In addition, the tensor
             structure of the Higgs boson couplings is studied using an
             effective Lagrangian approach for the description of
             interactions beyond the Standard Model. Constraints are
             placed on the non-Standard-Model CP-even and CP-odd
             couplings to Z bosons and on the CP-odd coupling to
             gluons.[Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP03(2018)095},
   Key = {fds356693}
}

@article{fds310360,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abidi, SH and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the Higgs boson mass from the H → γγ and
             H → ZZ- 4ℓ channels inpp collisions at
             center-of-mass energies of 7 and 8 TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.052004},
   Abstract = {An improved measurement of the mass of the Higgs boson is
             derived from a combined fit to the reconstructed invariant
             mass spectra of the decay channels H → γγ and H →
             ZZ∗→ 4ℓ. The analysis uses the pp collision data
             sample recorded by the ATLAS experiment at the CERN Large
             Hadron Collider at center-of-mass energies of 7 TeV and 8
             TeV, corresponding to an integrated luminosity of 25 fb-1.
             The measured value of the Higgs boson mass is mH= 125.36 ±
             0.37(stat) ± 0.18(syst) GeV. This result is based on
             improved energy-scale calibrations for photons, electrons,
             and muons as well as other analysis improvements, and
             supersedes the previous result from ATLAS. Upper limits on
             the total width of the Higgs boson are derived from fits to
             the invariant mass spectra of the H → γγ and H →
             ZZ∗→ 4ℓ decay channels.},
   Doi = {10.1103/PhysRevD.90.052004},
   Key = {fds310360}
}

@article{fds356662,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Measurement of the Higgs boson mass in the
             H → ZZ → 4ℓ and H → γγ
             channels with s=13 TeV pp collisions using the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {784},
   Pages = {345-366},
   Year = {2018},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.07.050},
   Abstract = {The mass of the Higgs boson is measured in the
             H→ZZ⁎→4ℓ and in the H→γγ decay channels with
             36.1 fb−1 of proton–proton collision data from the Large
             Hadron Collider at a centre-of-mass energy of 13 TeV
             recorded by the ATLAS detector in 2015 and 2016. The
             measured value in the H→ZZ⁎→4ℓ channel is
             mHZZ⁎=124.79±0.37GeV, while the measured value in the
             H→γγ channel is mHγγ=124.93±0.40GeV. Combining these
             results with the ATLAS measurement based on 7 and 8 TeV
             proton–proton collision data yields a Higgs boson mass of
             mH=124.97±0.24GeV.},
   Doi = {10.1016/j.physletb.2018.07.050},
   Key = {fds356662}
}

@article{fds372123,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V},
   Title = {Measurement of the Higgs boson mass in the
             H → ZZ → 4ℓ decay channel using
             139 fb−1 of s=13 TeV pp collisions recorded by
             the ATLAS detector at the LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {843},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.137880},
   Abstract = {The mass of the Higgs boson is measured in the
             H→ZZ⁎→4ℓ decay channel. The analysis uses
             proton–proton collision data from the Large Hadron
             Collider at a centre-of-mass energy of 13 TeV recorded by
             the ATLAS detector between 2015 and 2018, corresponding to
             an integrated luminosity of 139 fb−1. The measured value
             of the Higgs boson mass is 124.99±0.18(stat.)±0.04(syst.)
             GeV. In final states with muons, this measurement benefits
             from an improved momentum-scale calibration relative to that
             adopted in previous publications. The measurement also
             employs an analytic model that takes into account the
             invariant-mass resolution of the four-lepton system on a
             per-event basis and the output of a deep neural network
             discriminating signal from background events. This
             measurement is combined with the corresponding measurement
             using 7 and 8 TeV pp collision data, resulting in a Higgs
             boson mass of 124.94±0.17(stat.)±0.03(syst.)
             GeV.},
   Doi = {10.1016/j.physletb.2023.137880},
   Key = {fds372123}
}

@article{fds375875,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
             SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
             CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
   Title = {Measurement of the Higgs boson mass with H → γγ
             decays in 140 fb−1 of s=13 TeV pp collisions
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {847},
   Year = {2023},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.138315},
   Abstract = {The mass of the Higgs boson is measured in the H→γγ
             decay channel, exploiting the high resolution of the
             invariant mass of photon pairs reconstructed from the decays
             of Higgs bosons produced in proton–proton collisions at a
             centre-of-mass energy s=13 TeV. The dataset was collected
             between 2015 and 2018 by the ATLAS detector at the Large
             Hadron Collider, and corresponds to an integrated luminosity
             of 140 fb−1. The measured value of the Higgs boson mass is
             125.17±0.11(stat.)±0.09(syst.) GeV and is based on an
             improved energy scale calibration for photons, whose impact
             on the measurement is about four times smaller than in the
             previous publication. A combination with the corresponding
             measurement using 7 and 8 TeV pp collision ATLAS data
             results in a Higgs boson mass measurement of
             125.22±0.11(stat.)±0.09(syst.) GeV. With an uncertainty of
             1.1 per mille, this is currently the most precise
             measurement of the mass of the Higgs boson from a single
             decay channel.},
   Doi = {10.1016/j.physletb.2023.138315},
   Key = {fds375875}
}

@article{fds308216,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon,
             R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland,
             T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E},
   Title = {Measurement of the high-mass drell-yan cross section and
             limits on quark-electron compositeness scales},
   Journal = {Physical Review Letters},
   Volume = {82},
   Number = {24},
   Pages = {4769-4774},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.82.4769},
   Abstract = {We present a measurement of the Drell-Yan cross section at
             high dielectron invariant mass using 120 pb-1 of data
             collected in pp collisions at √ s = 1.8 TeV by the D0
             Collaboration during 1992-1996. No deviation from standard
             model expectations is observed. We use the data to set
             limits on the quark-electron compositeness scale. The 95%
             confidence level lower limits on the compositeness scale
             vary between 3.3 and 6.1 TeV depending on the assumed form
             of the effective contact interaction. © 1999 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.82.4769},
   Key = {fds308216}
}

@article{fds307647,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Measurement of the high-mass Drell–Yan differential
             cross-section in pp collisions at √s=7TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {725},
   Number = {4-5},
   Pages = {223-242},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.07.049},
   Abstract = {This Letter reports a measurement of the high-mass
             Drell–Yan differential cross-section in proton–proton
             collisions at a centre-of-mass energy of 7 TeV at the LHC.
             Based on an integrated luminosity of 4.9 fb−1, the
             differential cross-section in the Z/γ⁎→e+e− channel
             is measured with the ATLAS detector as a function of the
             invariant mass, mee, in the range 116 <mee <1500 GeV, for a
             fiducial region in which both the electron and the positron
             have transverse momentum pT >25 GeV and pseudorapidity |η|
             <2.5. A comparison is made to various event generators and
             to the predictions of perturbative QCD calculations at
             next-to-next-to-leading order.},
   Doi = {10.1016/j.physletb.2013.07.049},
   Key = {fds307647}
}

@article{fds375363,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye,
             T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal,
             A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja,
             S and Ai, X and Aielli, G and Aikot, A and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
             SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
             AA and Cardoso, MA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler,
             A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Dos Santos,
             SPA and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA},
   Title = {Measurement of the H→ γγ and H→ ZZ→ 4
             ℓ cross-sections in pp collisions at √s=13.6 TeV with
             the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {84},
   Number = {1},
   Year = {2024},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-12130-5},
   Abstract = {The inclusive Higgs boson production cross-section is
             measured in the di-photon and the ZZ∗→ 4 ℓ decay
             channels using 31.4 and 29.0 fb - 1 of pp collision data
             respectively, collected with the ATLAS detector at a
             centre-of-mass energy of s=13.6 TeV . To reduce the model
             dependence, the measurement in each channel is restricted to
             a particle-level phase space that closely matches the
             channel’s detector-level kinematic selection, and it is
             corrected for detector effects. These measured fiducial
             cross-sections are σfid,γγ= 76-13+14 fb, and σfid,4ℓ=
             2.80±0.74 fb, in agreement with the corresponding Standard
             Model predictions of 67.6 ± 3.7 fb and 3.67 ± 0.19 fb.
             Assuming Standard Model acceptances and branching fractions
             for the two channels, the fiducial measurements are
             extrapolated to the full phase space yielding total
             cross-sections of σ(pp→H)=67-11+12 pb and 46 ± 12 pb at
             13.6 TeV from the di-photon and ZZ∗→ 4 ℓ measurements
             respectively. The two measurements are combined into a total
             cross-section measurement of σ(pp→ H) = 58.2 ± 8.7 pb,
             to be compared with the Standard Model prediction of
             σ(pp→ H) SM= 59.9 ± 2.6 pb.},
   Doi = {10.1140/epjc/s10052-023-12130-5},
   Key = {fds375363}
}

@article{fds325309,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, A and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amoros, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antosb, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
             G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchou, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
             N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Boeser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler,
             S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans,
             G and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Buescher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth,
             JM and Buttinger, W and Byatt, T and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
             R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito,
             L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
             X and Cheng, S and Cheplakov, A and Chepurnov, VF and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG},
   Title = {Measurement of the inclusive and dijet cross-sections of
             b-jets in pp collisions at √s=7 TeV
             with the ATLAS detector},
   Journal = {EUROPEAN PHYSICAL JOURNAL C},
   Volume = {71},
   Number = {12},
   Publisher = {Springer New York LLC},
   Year = {2011},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1846-4},
   Abstract = {The inclusive and dijet production cross-sections have been
             measured for jets containing b-hadrons (b-jets) in
             proton-proton collisions at a centre-of-mass energy of +fs =
             7 TeV, using the ATLAS detector at the LHC. The measurements
             use data corresponding to an integrated luminosity of 34
             pb_1. The b-jets are identified using either a
             lifetime-based method, where secondary decay vertices of
             b-hadrons in jets are reconstructed using information from
             the tracking detectors, or a muon-based method where the
             presence of a muon is used to identify semileptonic decays
             of b-hadrons inside jets. The inclusive b-jet cross-section
             is measured as a function of transverse momentum in the
             range 20 < pT < 400 GeV and rapidity in the range \y\ < 2.1.
             The bb-dijet cross-section is measured as a function of the
             dijet invariant mass in the range 110 < mjj < 760 GeV, the
             azimuthal angle difference between the two jets and the
             angular variable χ in two dijet mass regions. The results
             are compared with next-to-leading-order QCD predictions.
             Good agreement is observed between the measured
             cross-sections and the predictions obtained using POWHEG +
             Pythia. MC@NLO + Herwig shows good agreement with the
             measured bb-dijet cross-section. However, it does not
             reproduce the measured inclusive cross-section well,
             particularly for central b-jets with large transverse
             momenta.},
   Doi = {10.1140/epjc/s10052-011-1846-4},
   Key = {fds325309}
}

@article{fds347477,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
             C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
             AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
             O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
             R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
             JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M},
   Title = {Measurement of the inclusive and fiducial t t ¯ production
             cross-sections in the lepton+jets channel in pp
             collisions at s = 8 TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {6},
   Pages = {487},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-5904-z},
   Abstract = {The inclusive and fiducial t t ¯ production cross-sections
             are measured in the lepton+jets channel using 20.2 fb - 1 of
             proton-proton collision data at a centre-of-mass energy of 8
             TeV recorded with the ATLAS detector at the LHC. Major
             systematic uncertainties due to the modelling of the jet
             energy scale and <i>b</i>-tagging efficiency are constrained
             by separating selected events into three disjoint regions.
             In order to reduce systematic uncertainties in the most
             important background, the W +\,jets process is modelled
             using Z + jets events in a data-driven approach. The
             inclusive t t ¯ cross-section is measured with a precision
             of 5.7% to be σ inc ( t t ¯ ) = 248.3 ± 0.7 ( stat . ) ±
             13.4 ( syst . ) ± 4.7 ( lumi . ) pb , assuming a top-quark
             mass of 172.5 GeV. The result is in agreement with the
             Standard Model prediction. The cross-section is also
             measured in a phase space close to that of the selected
             data. The fiducial cross-section is σ fid ( t t ¯ ) = 48.8
             ± 0.1 ( stat . ) ± 2.0 ( syst . ) ± 0.9 ( lumi . ) pb
             with a precision of 4.5%.},
   Doi = {10.1140/epjc/s10052-018-5904-z},
   Key = {fds347477}
}

@article{fds356566,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
             V},
   Title = {Measurement of the inclusive cross-section for the
             production of jets in association with a Z boson in
             proton–proton collisions at 8 TeV using the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {10},
   Year = {2019},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7321-3},
   Abstract = {The inclusive cross-section for jet production in
             association with a Z boson decaying into an
             electron–positron pair is measured as a function of the
             transverse momentum and the absolute rapidity of jets using
             19.9 fb- 1 of s=8 TeV proton–proton collision data
             collected with the ATLAS detector at the Large Hadron
             Collider. The measured Z+ jets cross-section is unfolded to
             the particle level. The cross-section is compared with
             state-of-the-art Standard Model calculations, including the
             next-to-leading-order and next-to-next-to-leading-order
             perturbative QCD calculations, corrected for
             non-perturbative and QED radiation effects. The results of
             the measurements cover final-state jets with transverse
             momenta up to 1 TeV, and show good agreement with
             fixed-order calculations.},
   Doi = {10.1140/epjc/s10052-019-7321-3},
   Key = {fds356566}
}

@article{fds356754,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
             YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
             S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Armitage, LJ and Arnaez, O},
   Title = {Measurement of the inclusive cross-sections of single
             top-quark and top-antiquark t-channel production in pp
             collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {4},
   Year = {2017},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2017)086},
   Abstract = {A measurement of the t-channel single-top-quark and
             single-top-antiquark production cross-sections in the
             lepton+jets channel is presented, using 3.2 fb−1 of
             proton-proton collision data at a centre-of-mass energy of
             13 TeV, recorded with the ATLAS detector at the LHC in 2015.
             Events are selected by requiring one charged lepton
             (electron or muon), missing transverse momentum, and two
             jets with high transverse momentum, exactly one of which is
             required to be b-tagged. Using a binned maximum-likelihood
             fit to the discriminant distribution of a neural network,
             the cross-sections are determined to be σ(tq) = 156 ± 5
             (stat.) ± 27 (syst.) ± 3 (lumi.) pb for single top-quark
             production and σ(t¯ q) = 91 ± 4 (stat.) ± 18 (syst.) ±
             2 (lumi.) pb for single top-antiquark production, assuming a
             top-quark mass of 172.5 GeV. The cross-section ratio is
             measured to be Rt=σ(tq)/σ(t¯q)=1.72±0.09 (stat.) ± 0.18
             (syst.). All results are in agreement with Standard Model
             predictions.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP04(2017)086},
   Key = {fds356754}
}

@article{fds308196,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evans, H and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk,
             HE and Fisyak, Y and Flattum, E},
   Title = {Measurement of the inclusive differential cross section for
             Z bosons as a function of transverse momentum in [formula
             presented] collisions at [formula presented]
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {61},
   Number = {3},
   Pages = {1-19},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.61.032004},
   Abstract = {We present a measurement of the differential cross section
             as a function of transverse momentum of the Z boson in
             (Formula presented) collisions at (Formula presented) TeV
             using data collected by the DØ experiment at the Fermilab
             Tevatron Collider during 1994–1996. We find good agreement
             between our data and the next-to-next-to-next-leading-logarithmic
             resummation prediction and extract values of the
             non-perturbative parameters for the resummed prediction from
             a fit to the differential cross section. © 2000 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.61.032004},
   Key = {fds308196}
}

@article{fds373463,
   Author = {Jackson, P and Oliver, JL and Petridis, A and Qureshi, A and Sharma, AS and White, MJ and Cairo, VMM and Jain, V and Swift, SP and Gingrich, DM and Pinfold, JL and Sun, X and Wang, H and Cakir, O and Yildiz, HD and Kuday,
             S and Turk Cakir and I and Sultansoy, S and Berger, N and Costanza, F and Dartsi, O and Delmastro, M and Di Ciaccio and L and Falke, PJ and Falke, S and Goy, C and Guillemin, T and Hryn’ova, T and Jézéquel, S and Kivernyk, O and Koletsou, I and Lafaye, R and Levêque, J and Lorenzo
             Martinez, N and Raspopov, S and Sauvan, E and Smart, BH and Todorova-Nova, S and Vallier, A and Wingerter-Seez, I and Abulaiti,
             Y and Benjamin, DP and Chekanov, S and Hopkins, WH and LeCompte, T and Liu,
             BX and Love, J and Malon, D and Metcalfe, J and Paramonov, A and Proudfoot,
             J and Ryu, S and Stanek, RW and Van Gemmeren and P and Wang, R and Zhang, J and Berlendis, S and Cheu, E and Delitzsch, CM and Johns, KA and Jones, S and Lampl, W and LeBlanc, M and Leone, R and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and De, K and Farbin, A and Griffiths, J and Hadavand, HK and Heelan, L and Little,
             JD and Ozturk, N and Usai, G and White, A and Bellos, P and Fassouliotis,
             D and Gkialas, I and Kourkoumelis, C and Papageorgiou, K and Tsirintanis, N and Alexopoulos, T and Bakalis, C and Benekos, N and Gazis, EN and Gkountoumis, P and Koulouris, A and Maltezos, S and Moschovakos, P and Panagoulias, I and Zacharis, G and Andeen, T and Narayan, R and Nikiforou, N and Onyisi, PUE and Potti,
             H},
   Title = {Measurement of the inclusive Formula Presented production
             cross section in the lepton+jets channel in pp collisions at
             Formula Presented with the ATLAS detector using support
             vector machines},
   Journal = {Physical Review D},
   Volume = {108},
   Number = {3},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.108.032014},
   Abstract = {A measurement of the top quark pair-production cross section
             in the lepton + jets decay channel is presented. It is based
             on 4.6 fb - 1 of s = 7 TeV p p collision data collected
             during 2011 by the ATLAS experiment at the CERN Large Hadron
             Collider. A three-class, multidimensional event classifier
             based on support vector machines is used to differentiate t
             t ¯ events from backgrounds. The t t ¯ production cross
             section is found to be σ t t ¯ = 168.5 ± 0.7 ( stat ) -
             5.9 + 6.2 ( syst ) - 3.2 + 3.4 ( lumi ) pb . The result is
             consistent with the Standard Model prediction based on QCD
             calculations at next-to-next-to-leading order.},
   Doi = {10.1103/PhysRevD.108.032014},
   Key = {fds373463}
}

@article{fds307999,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the inclusive isolated prompt photon cross
             section in $pp[over \ifmmode\bar\else\textasciimacron\fi{}]$
             collisions at $\sqrt{s}=1.96\,\,TeV$ using the CDF
             detector},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {11},
   Pages = {111106},
   Publisher = {American Physical Society},
   Year = {2009},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.111106},
   Abstract = {A measurement of the cross section for the inclusive
             production of isolated photons by the CDF experiment at the
             Fermilab Tevatron collider is presented. The measurement
             covers the pseudorapidity region $|\eta\gamma|30$  GeV
             and is based on 2.5  fb-1 of integrated luminosity. The
             sample is almost a factor of 7 larger than those used for
             recent published results and extends the $E_T^\gamma$
             coverage by 100 GeV. The result agrees with next-to-leading
             order perturbative QCD calculations within uncertainties
             over the range $50},
   Doi = {10.1103/PhysRevD.80.111106},
   Key = {fds307999}
}

@article{fds321105,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold,
             H},
   Title = {Measurement of the inclusive isolated prompt photon cross
             section in pp collisions at s=8TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2016)005},
   Abstract = {Abstract: A measurement of the cross section for the
             inclusive production of isolated prompt photons in
             proton-proton collisions at a centre-of-mass energy of s=8
             TeV is presented. The measurement covers the pseudorapidity
             ranges |ηγ | < 1.37 and 1.56 ≤ |ηγ | < 2.37 in the
             transverse energy range 25 < ETγ < 1500 GeV. The results
             are based on an integrated luminosity of 20.2 fb−1,
             recorded by the ATLAS detector at the LHC. Photon candidates
             are identified by combining information from the
             calorimeters and the inner tracker. The background is
             subtracted using a data-driven technique, based on the
             observed calorimeter shower-shape variables and the
             deposition of hadronic energy in a narrow cone around the
             photon candidate. The measured cross sections are compared
             with leading-order and next-to-leading order perturbative
             QCD calculations and are found to be in a good agreement
             over ten orders of magnitude.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP08(2016)005},
   Key = {fds321105}
}

@article{fds307857,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the inclusive isolated prompt photon
             cross-section in pp collisions at √s=7 TeV using 35
             pb-1 of ATLAS data},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {706},
   Number = {2-3},
   Pages = {150-167},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.11.010},
   Abstract = {A measurement of the differential cross-section for the
             inclusive production of isolated prompt photons in pp
             collisions at a center-of-mass energy √s=7 TeV is
             presented. The measurement covers the pseudorapidity ranges
             |η|<1.37 and 1.52≤|η|<2.37 in the transverse energy
             range 45≤ET<400 GeV. The results are based on an
             integrated luminosity of 35 pb-1, collected with the ATLAS
             detector at the LHC. The yields of the signal photons are
             measured using a data-driven technique, based on the
             observed distribution of the hadronic energy in a narrow
             cone around the photon candidate and the photon selection
             criteria. The results are compared with next-to-leading
             order perturbative QCD calculations and found to be in good
             agreement over four orders of magnitude in cross-section. ©
             2011 CERN.},
   Doi = {10.1016/j.physletb.2011.11.010},
   Key = {fds307857}
}

@article{fds307548,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {Measurement of the inclusive isolated prompt photons cross
             section in pp collisions at √s =7 TeV with the ATLAS
             detector using 4.6 fb-1},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.052004},
   Abstract = {A measurement of the cross section for the production of
             isolated prompt photons in pp collisions at a center-of-mass
             energy √s=7 TeV is presented. The results are based on an
             integrated luminosity of 4.6 fb-1 collected with the ATLAS
             detector at the LHC. The cross section is measured as a
             function of photon pseudorapidity ηγ and transverse energy
             ETγ in the kinematic range 100≤ETγ<1000 GeV and in the
             regions |ηγ|<1.37 and 1.52≤|ηγ|<2.37. The results are
             compared to leading-order parton-shower Monte Carlo models
             and next-to-leading-order perturbative QCD calculations.
             Next-to-leading-order perturbative QCD calculations agree
             well with the measured cross sections as a function of ETγ
             and ηγ.},
   Doi = {10.1103/PhysRevD.89.052004},
   Key = {fds307548}
}

@article{fds356569,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
             V},
   Title = {Measurement of the inclusive isolated-photon cross section
             in pp collisions at √s = 13 TeV using 36 fb−1
             of ATLAS data},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {10},
   Year = {2019},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2019)203},
   Abstract = {The differential cross section for isolated-photon
             production in pp collisions is measured at a centre-of-mass
             energy of 13 TeV with the ATLAS detector at the LHC using an
             integrated luminosity of 36.1 fb−1. The differential cross
             section is presented as a function of the photon transverse
             energy in different regions of photon pseudorapidity. The
             differential cross section as a function of the absolute
             value of the photon pseudorapidity is also presented in
             different regions of photon transverse energy.
             Next-to-leading-order QCD calculations from Jetphox and
             Sherpa as well as next-to-next-to-leading-order QCD
             calculations from Nnlojet are compared with the measurement,
             using several parameterisations of the proton parton
             distribution functions. The predictions provide a good
             description of the data within the experimental and
             theoretical uncertainties. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP10(2019)203},
   Key = {fds356569}
}

@article{fds308112,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the inclusive jet cross section in ppbar
             Interactions at sqrt{s}=1.96 TeV Using a Cone-based Jet
             Algorithm},
   Journal = {Phys. Rev.},
   Volume = {D74},
   Number = {7},
   Pages = {071103},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.74.071103},
   Abstract = {We present a measurement of the inclusive jet cross section
             in ppbar interactions at sqrt{s}=1.96 TeV using 385 pb^{-1}
             of data collected with the CDF II detector at the Fermilab
             Tevatron. The results are obtained using an improved
             cone-based jet algorithm (Midpoint). The data cover the jet
             transverse momentum range from 61 to 620 GeV/c, extending
             the reach by almost 150 GeV/c compared with previous
             measurements at the Tevatron. The results are in good
             agreement with next-to-leading order perturbative QCD
             predictions using the CTEQ6.1M parton distribution
             functions.},
   Doi = {10.1103/PhysRevD.74.071103},
   Key = {fds308112}
}

@article{fds308099,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the inclusive jet cross section using the
             k(t) algorithm in p anti-p collisions at $\sqrt{s}=$ 1.96-
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {12},
   Pages = {122001},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.122001},
   Abstract = {We report on a measurement of the inclusive jet production
             cross section in p anti-p collisions at s**(1/2) = 1.96 TeV
             using data collected with the upgraded Collider Detector at
             Fermilab in Run II (CDF II) corresponding to an integrated
             luminosity of 385 pb-1. Jets are reconstructed using the K_T
             algorithm. The measurement is carried out for jets with
             rapidity $0.1},
   Doi = {10.1103/physrevlett.96.122001},
   Key = {fds308099}
}

@article{fds308075,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
             M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
             MA},
   Title = {Measurement of the inclusive jet cross section using the kT
             algorithm in pp̄ collisions at s=1.96TeV with the CDF II
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {75},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.092006},
   Abstract = {We report on measurements of the inclusive jet production
             cross section as a function of the jet transverse momentum
             in pp̄ collisions at s=1.96TeV, using the kT algorithm and
             a data sample corresponding to 1.0fb-1 collected with the
             Collider Detector at Fermilab in run II. The measurements
             are carried out in five different jet rapidity regions with
             |yjet|<2.1 and transverse momentum in the range
             54<pTjet<700GeV/c. Next-to-leading order perturbative QCD
             predictions are in good agreement with the measured cross
             sections. © 2007 The American Physical Society.},
   Doi = {10.1103/PhysRevD.75.092006},
   Key = {fds308075}
}

@article{fds307588,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, KM and Blair,
             RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm,
             J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
             S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez
             Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
             A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A},
   Title = {Measurement of the inclusive jet cross-section in pp
             collisions at [Formula: see text] and comparison to the
             inclusive jet cross-section at [Formula: see text] using the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {8},
   Pages = {2509},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2509-4},
   Abstract = {The inclusive jet cross-section has been measured in
             proton-proton collisions at [Formula: see text] in a dataset
             corresponding to an integrated luminosity of [Formula: see
             text] collected with the ATLAS detector at the Large Hadron
             Collider in 2011. Jets are identified using the
             anti-<i>k</i><sub><i>t</i></sub> algorithm with two radius
             parameters of 0.4 and 0.6. The inclusive jet
             double-differential cross-section is presented as a function
             of the jet transverse momentum <i>p</i><sub>T</sub> and jet
             rapidity <i>y</i>, covering a range of 20≤<i>p</i><sub>T</sub><430 GeV
             and |<i>y</i>|<4.4. The ratio of the cross-section to the
             inclusive jet cross-section measurement at [Formula: see
             text], published by the ATLAS Collaboration, is calculated
             as a function of both transverse momentum and the
             dimensionless quantity [Formula: see text], in bins of jet
             rapidity. The systematic uncertainties on the ratios are
             significantly reduced due to the cancellation of correlated
             uncertainties in the two measurements. Results are compared
             to the prediction from next-to-leading order perturbative
             QCD calculations corrected for non-perturbative effects, and
             next-to-leading order Monte Carlo simulation. Furthermore,
             the ATLAS jet cross-section measurements at [Formula: see
             text] and [Formula: see text] are analysed within a
             framework of next-to-leading order perturbative QCD
             calculations to determine parton distribution functions of
             the proton, taking into account the correlations between the
             measurements.},
   Doi = {10.1140/epjc/s10052-013-2509-4},
   Key = {fds307588}
}

@article{fds310305,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the inclusive jet cross-section in
             proton-proton collisions at √s=7 TeV using 4.5
             fb−1 of data with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {2},
   Pages = {1-54},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP02(2015)153},
   Abstract = {Abstract: The inclusive jet cross-section is measured in
             proton-proton collisions at a centre-of-mass energy of 7 TeV
             using a data set corresponding to an integrated luminosity
             of 4.5 fb−1 collected with the ATLAS detector at the Large
             Hadron Collider in 2011. Jets are identified using the
             anti-kt algorithm with radius parameter values of 0.4 and
             0.6. The double-differential cross-sections are presented as
             a function of the jet transverse momentum and the jet
             rapidity, covering jet transverse momenta from 100 GeV to 2
             TeV. Next-to-leading-order QCD calculations corrected for
             non-perturbative effects and electroweak effects, as well as
             Monte Carlo simulations with next-to-leading-order matrix
             elements interfaced to parton showering, are compared to the
             measured cross-sections. A quantitative comparison of the
             measured cross-sections to the QCD calculations using
             several sets of parton distribution functions is
             performed.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP02(2015)153},
   Key = {fds310305}
}

@article{fds356736,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
             LJ},
   Title = {Measurement of the inclusive jet cross-sections in
             proton-proton collisions at √s=8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {9},
   Year = {2017},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2017)020},
   Abstract = {Inclusive jet production cross-sections are measured in
             proton-proton collisions at a centre-of-mass energy of s=8
             TeV recorded by the ATLAS experiment at the Large Hadron
             Collider at CERN. The total integrated luminosity of the
             analysed data set amounts to 20.2 fb−1.
             Double-differential cross-sections are measured for jets
             defined by the anti-kt jet clustering algorithm with radius
             parameters of R = 0.4 and R = 0.6 and are presented as a
             function of the jet transverse momentum, in the range
             between 70 GeV and 2.5 TeV and in six bins of the absolute
             jet rapidity, between 0 and 3.0. The measured cross-sections
             are compared to predictions of quantum chromodynamics,
             calculated at next-to-leading order in perturbation theory,
             and corrected for non-perturbative and electroweak effects.
             The level of agreement with predictions, using a selection
             of different parton distribution functions for the proton,
             is quantified. Tensions between the data and the theory
             predictions are observed.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP09(2017)020},
   Key = {fds356736}
}

@article{fds310371,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Henry, S and Herndon,
             M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
             JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
             M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
             G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
             A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
             P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese,
             L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta,
             A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra,
             A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia,
             E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
             J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St
             Denis, R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
             P and Wallny, R and Wang, SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of the inclusive leptonic asymmetry in top-quark
             pairs that decay to two charged leptons at
             CDF.},
   Journal = {Physical review letters},
   Volume = {113},
   Number = {4},
   Pages = {042001},
   Year = {2014},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.113.042001},
   Abstract = {We measure the inclusive forward-backward asymmetry of the
             charged-lepton pseudorapidities from top-quark pairs
             produced in proton-antiproton collisions and decaying to
             final states that contain two charged leptons (electrons or
             muons). The data are collected with the Collider Detector at
             Fermilab and correspond to an integrated luminosity of 9.1
             fb(-1). We measure the leptonic forward-backward asymmetry,
             A(FB)(ℓ), to be 0.072 ± 0.060 and the leptonic pair
             forward-backward asymmetry, A(FB)(ℓℓ), to be 0.076 ±
             0.082. The measured values can be compared with the standard
             model predictions of A(FB)(ℓ) = 0.038 ± 0.003 and
             A(FB)(ℓℓ) = 0.048 ± 0.004, respectively. Additionally,
             we combine the A(FB)(ℓ) result with a previous
             determination from a final state with a single lepton and
             hadronic jets and obtain A(FB)(ℓ) = 0.090(-0.026)(+0.028).},
   Doi = {10.1103/physrevlett.113.042001},
   Key = {fds310371}
}

@article{fds307742,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the inclusive W± and Z/γ∗
             cross sections in the e and μ decay channels in pp
             collisions at √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.072004},
   Abstract = {The production cross sections of the inclusive Drell-Yan
             processes W ±→ν and Z/γ∗→(=e, μ) are measured in
             proton-proton collisions at √s=7TeV with the ATLAS
             detector. The cross sections are reported integrated over a
             fiducial kinematic range, extrapolated to the full range,
             and also evaluated differentially as a function of the W
             decay lepton pseudorapidity and the Z boson rapidity,
             respectively. Based on an integrated luminosity of about
             35pb-1 collected in 2010, the precision of these
             measurements reaches a few percent. The integrated and the
             differential W± and Z/γ∗ cross sections in the e and μ
             channels are combined, and compared with perturbative QCD
             calculations, based on a number of different parton
             distribution sets available at next-to-next-to-leading
             order.},
   Doi = {10.1103/PhysRevD.85.072004},
   Key = {fds307742}
}

@article{fds356722,
   Author = {Aaltonen, T and Albrow, MG and Amerio, S and Amidei, D and Anastassov,
             A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
             T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri,
             A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
             B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
             A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
             F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
             DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'errico, M and Devoto, F and Di Canto and A and Di Ruzza,
             B and Dittmann, JR and Donati, S and D'onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Erbacher, R and Errede,
             S},
   Title = {Measurement of the inclusive-isolated prompt-photon cross
             section in pp collisions using the full CDF data
             set},
   Journal = {Physical Review D},
   Volume = {96},
   Number = {9},
   Year = {2017},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.96.092003},
   Abstract = {A measurement of the inclusive production cross section of
             isolated prompt photons in proton-antiproton collisions at
             center-of-mass energy s=1.96 TeV is presented. The results
             are obtained using the full Run II data sample collected
             with the Collider Detector at the Fermilab Tevatron, which
             corresponds to an integrated luminosity of 9.5 fb-1. The
             cross section is measured as a function of photon transverse
             energy, ETγ, in the range 30<ETγ<500 GeV and in the
             pseudorapidity region |ηγ|<1.0. The results are compared
             with predictions from parton-shower Monte Carlo models at
             leading order in QCD and from next-to-leading-order
             perturbative QCD calculations. The latter show good
             agreement with the measured cross section.},
   Doi = {10.1103/PhysRevD.96.092003},
   Key = {fds356722}
}

@article{fds321080,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
             K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
             J and Billoud, TRV and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
             Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M},
   Title = {Measurement of the Inelastic Proton-Proton Cross Section at
             sqrt[s]=13  TeV with the ATLAS Detector at the
             LHC.},
   Journal = {Phys Rev Lett},
   Volume = {117},
   Number = {18},
   Pages = {182002},
   Year = {2016},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevLett.117.182002},
   Abstract = {This Letter presents a measurement of the inelastic
             proton-proton cross section using 60  μb^{-1} of pp
             collisions at a center-of-mass energy sqrt[s] of 13 TeV
             with the ATLAS detector at the LHC. Inelastic interactions
             are selected using rings of plastic scintillators in the
             forward region (2.07<|η|<3.86) of the detector. A cross
             section of 68.1±1.4  mb is measured in the fiducial
             region ξ=M_{X}^{2}/s>10^{-6}, where M_{X} is the larger
             invariant mass of the two hadronic systems separated by the
             largest rapidity gap in the event. In this ξ range the
             scintillators are highly efficient. For diffractive events
             this corresponds to cases where at least one proton
             dissociates to a system with M_{X}>13  GeV. The measured
             cross section is compared with a range of theoretical
             predictions. When extrapolated to the full phase space, a
             cross section of 78.1±2.9  mb is measured, consistent
             with the inelastic cross section increasing with
             center-of-mass energy.},
   Doi = {10.1103/PhysRevLett.117.182002},
   Key = {fds321080}
}

@article{fds321140,
   Author = {ATLAS Collaboration},
   Title = {Measurement of the inelastic proton-proton cross-section at
             √s=7 TeV with the ATLAS detector.},
   Journal = {Nature communications},
   Volume = {2},
   Number = {1},
   Pages = {463},
   Year = {2011},
   Month = {September},
   url = {http://dx.doi.org/10.1038/ncomms1472},
   Abstract = {The dependence of the rate of proton-proton interactions on
             the centre-of-mass collision energy, √s, is of fundamental
             importance for both hadron collider physics and particle
             astrophysics. The dependence cannot yet be calculated from
             first principles; therefore, experimental measurements are
             needed. Here we present the first measurement of the
             inelastic proton-proton interaction cross-section at a
             centre-of-mass energy, √s, of 7 TeV using the ATLAS
             detector at the Large Hadron Collider. Events are selected
             by requiring hits on scintillation counters mounted in the
             forward region of the detector. An inelastic cross-section
             of 60.3 ± 2.1 mb is measured for ξ > 5×10⁻⁶, where ξ
             is calculated from the invariant mass, M(X), of hadrons
             selected using the largest rapidity gap in the event. For
             diffractive events, this corresponds to requiring at least
             one of the dissociation masses to be larger than 15.7
             GeV.},
   Doi = {10.1038/ncomms1472},
   Key = {fds321140}
}

@article{fds307744,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Measurement of the isolated diphoton cross section in pp
             collisions at √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012003},
   Abstract = {The ATLAS experiment has measured the production cross
             section of events with two isolated photons in the final
             state, in proton-proton collisions at √s=7TeV. The full
             data set acquired in 2010 is used, corresponding to an
             integrated luminosity of 37pb -1. The background, consisting
             of hadronic jets and isolated electrons, is estimated with
             fully data-driven techniques and subtracted. The
             differential cross sections, as functions of the di-photon
             mass (m γγ), total transverse momentum (p T,γγ), and
             azimuthal separation (Δφ γγ), are presented and compared
             to the predictions of next-to-leading-order QCD. © 2012
             CERN.},
   Doi = {10.1103/PhysRevD.85.012003},
   Key = {fds307744}
}

@article{fds340913,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             L and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
             AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
             JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and DrollingerV, and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
             D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko,
             I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
             E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
             C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, V and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher,
             F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and HaywardH, and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and HoffmanK, D and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
             D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
             KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
             PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
             BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
             AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
             SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen,
             D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson,
             M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic,
             N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
             B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
             C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti,
             R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
             C and Pompoš, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman,
             D},
   Title = {Measurement of the J/ψ meson and b-hadron production cross
             sections in pp̄ collisions at √s = 1960
             GeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {3},
   Pages = {032001-1-032001-26},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.032001},
   Abstract = {We present a new measurement of the inclusive and
             differential production cross sections of J/ψ mesons and b
             hadrons in proton-antiproton collisions at √s = 1960 GeV.
             The data correspond to an integrated luminosity of 39.7 pb-1
             collected by the CDF run II detector. We find the integrated
             cross section for inclusive J/ψ production for all
             transverse momenta from 0 to 20 GeV/c in the rapidity range
             |y| &lt; 0.6 to be 4.08 ± 0.02(Stat)-0.33+0.36(syst) μb.
             We separate the fraction of J/ψ events from the decay of
             the long-lived b hadrons using the lifetime distribution in
             all events with pT(J/ψ) &gt; 1.25 GeV/c. We find the total
             cross section for b hadrons, including both hadrons and
             antihadrons, decaying to J/ψ with transverse momenta
             greater than 1.25 GeV/c in the rapidity range |y(J/ψ)| &lt;
             0.6 is 0.330 ± 0.005(stat) -0.033+0.036(syst) μb. Using a
             Monte Carlo simulation of the decay kinematics of b hadrons
             to all final states containing a J/ψ, we extract the first
             measurement of the total single b-hadron cross section down
             to zero transverse momentum at √s = 1960 GeV. We find the
             total single b-hadron cross section integrated over all
             transverse momenta for b hadrons in the rapidity range |y|
             &lt; 0.6 to be 17.6 ± 0.4(stat) -2.3+2.5(syst) μb. © 2005
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.71.032001},
   Key = {fds340913}
}

@article{fds310408,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the jet fragmentation function and transverse
             profile in proton–proton collisions at a center-of-mass
             energy of 7 TeV with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {December},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1795-y},
   Abstract = {The jet fragmentation function and transverse profile for
             jets with 25 GeV< pTjet < 500 GeV and |ηjet| < 1.2 produced
             in proton–proton collisions with a center-ofmass energy of
             7 TeV are presented. The measurement is performed using data
             with an integrated luminosity of 36 pb−1. Jets are
             reconstructed and their momentum measured using calorimetric
             information. The momenta of the charged particle
             constituents are measured using the tracking system. The
             distributions corrected for detector effects are compared
             with various Monte Carlo event generators and generator
             tunes. Several of these choices show good agreement with the
             measured fragmentation function. None of these choices
             reproduce both the transverse profile and fragmentation
             function over the full kinematic range of the
             measurement.},
   Doi = {10.1140/epjc/s10052-011-1795-y},
   Key = {fds310408}
}

@article{fds307626,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, R and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, E and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, R and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel,
             M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Belaboradova, O and Belotiskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Nocioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Bensalma, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitnec, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boviea, A and Boyd, J and Boyka, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, E and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Carbreara Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido,
             MDMC and Caprini, I and Caprini, M and Capriotti, D and Capau, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, E and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, E and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins,
             NJ and Collins-Tooth, C and Collot, J},
   Title = {Measurement of the jet radius and transverse momentum
             dependence of inclusive jet suppression in lead-lead
             collisions at √SNN=2.76 TeV with the
             ATLAS detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {719},
   Number = {4-5},
   Pages = {220-241},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.024},
   Abstract = {Measurements of inclusive jet suppression in heavy ion
             collisions at the LHC provide direct sensitivity to the
             physics of jet quenching. In a sample of lead–lead
             collisions at sNN=2.76 TeV corresponding to an integrated
             luminosity of approximately 7 μb−1, ATLAS has measured
             jets with a calorimeter system over the pseudorapidity
             interval |η|<2.1 and over the transverse momentum range
             38<pT<210 GeV. Jets were reconstructed using the anti-kt
             algorithm with values for the distance parameter that
             determines the nominal jet radius of R=0.2, 0.3, 0.4 and
             0.5. The centrality dependence of the jet yield is
             characterized by the jet “central-to-peripheral ratio,”
             RCP. Jet production is found to be suppressed by
             approximately a factor of two in the 10% most central
             collisions relative to peripheral collisions. RCP varies
             smoothly with centrality as characterized by the number of
             participating nucleons. The observed suppression is only
             weakly dependent on jet radius and transverse momentum.
             These results provide the first direct measurement of
             inclusive jet suppression in heavy ion collisions and
             complement previous measurements of dijet transverse energy
             imbalance at the LHC.},
   Doi = {10.1016/j.physletb.2013.01.024},
   Key = {fds307626}
}

@article{fds356744,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
             LJ},
   Title = {Measurement of the k t splitting scales in Z →
             ℓℓ events in pp collisions at √s=8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {8},
   Year = {2017},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2017)026},
   Abstract = {A measurement of the splitting scales occuring in the kt
             jet-clustering algorithm is presented for final states
             containing a Z boson. The measurement is done using 20.2
             fb−1 of proton-proton collision data collected at a
             centre-of-mass energy of s=8 TeV by the ATLAS experiment at
             the LHC in 2012. The measurement is based on chargedparticle
             track information, which is measured with excellent
             precision in the pT region relevant for the transition
             between the perturbative and the non-perturbative regimes.
             The data distributions are corrected for detector effects,
             and are found to deviate from state-of-the-art predictions
             in various regions of the observables.[Figure not available:
             see fulltext.].},
   Doi = {10.1007/JHEP08(2017)026},
   Key = {fds356744}
}

@article{fds307950,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the k[sub T] Distribution of Particles in
             Jets Produced in p[overline p] Collisions at sqrt(s) = 1.96
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {23},
   Pages = {232002},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.232002},
   Abstract = {We present a measurement of the transverse momentum with
             respect to the jet axis (k(t)) of particles in jets produced
             in pp collisions at sqrt(s)=1.96 TeV. Results are obtained
             for charged particles in a cone of 0.5 radians around the
             jet axis in events with dijet invariant masses between 66
             and 737 GeV/c(2). The experimental data are compared to
             theoretical predictions obtained for fragmentation partons
             within the framework of resummed perturbative QCD using the
             modified leading log and next-to-modified leading log
             approximations. The comparison shows that trends in data are
             successfully described by the theoretical predictions,
             indicating that the perturbative QCD stage of jet
             fragmentation is dominant in shaping basic jet
             characteristics.},
   Doi = {10.1103/physrevlett.102.232002},
   Key = {fds307950}
}

@article{fds307569,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Measurement of the leptonic asymmetry in tt̄ events
             produced in pp̄ collisions at √s=1.96
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {7},
   Pages = {072003},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.072003},
   Abstract = {We measure the asymmetry in the charge-weighted rapidity
             qyℓ of the lepton in semileptonic tt̄ decays recorded
             with the CDF II detector using the full Tevatron Run II
             sample, corresponding to an integrated luminosity of 9.4
             fb-1. A parametrization of the asymmetry as a function of
             qyℓ is used to correct for the finite acceptance of the
             detector and recover the production-level asymmetry. The
             result of AFBℓ=0.094-0.029+0.032 is to be compared to the
             standard model next-to-leading-order prediction of
             AFBℓ=0.038±0.003. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.88.072003},
   Key = {fds307569}
}

@article{fds308133,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, J-F and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
             JY and Chung, W-H and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
             AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Da Ronco and S and D'Auria, S and de Barbaro, P and De Cecco and S and De Lentdecker and G and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann,
             JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
             D and Errede, S and Eusebi, R and Fang, H-C and Farrington, S and Fedorko,
             I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
             E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
             C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and da Costa, JG and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
             M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
             H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko,
             S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko,
             I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann,
             SE and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu,
             R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller,
             L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
             B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
             C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti,
             R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
             C and Pompos, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and St Denis and R and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman,
             D},
   Title = {Measurement of the lifetime difference between Bs mass
             eigenstates.},
   Journal = {Physical review letters},
   Volume = {94},
   Number = {10},
   Pages = {101803},
   Year = {2005},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.94.101803},
   Abstract = {We present measurements of the lifetimes and polarization
             amplitudes for B(0)(s)-->J/psiphi and B(0)(d)-->J/psiK(*0)
             decays. Lifetimes of the heavy and light mass eigenstates in
             the B(0)(s) system are separately measured for the first
             time by determining the relative contributions of amplitudes
             with definite CP as a function of the decay time. Using
             203+/-15 B(0)(s) decays we obtain tau(L) =
             (1.05(+0.16)(-0.13) +/- 0.02) ps and tau(H) =
             (2.07(+0.58)(-0.46) +/- 0.03) ps. Expressed in terms of the
             difference DeltaGamma(s) and average Gamma(s), of the decay
             rates of the two eigenstates, the results are
             DeltaGamma(s)/Gamma(s) = (65(+25)(-33) +/- 1)% and
             DeltaGamma(s) = (0.47(+0.19)(-0.24) +/- 0.01)
             ps(-1).},
   Doi = {10.1103/physrevlett.94.101803},
   Key = {fds308133}
}

@article{fds310376,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Measurement of the low-mass Drell-Yan differential cross
             section at √s = 7 TeV using the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP06(2014)112},
   Abstract = {The differential cross section for the process Z/γ * →
             ℓℓ (ℓ = e, μ) as a function of dilepton invariant
             mass is measured in pp collisions at √s = 7 TeV at the LHC
             using the ATLAS detector. The measurement is performed in
             the e and μ channels for invariant masses between 26 GeV
             and 66 GeV using an integrated luminosity of 1.6 fb -1
             collected in 2011 and these measurements are combined. The
             analysis is extended to invariant masses as low as 12 GeV in
             the muon channel using 35 pb-1 of data collected in 2010.
             The cross sections are determined within fiducial acceptance
             regions and corrections to extrapolate the measurements to
             the full kinematic range are provided. Next-to-next-to-leading-
             order QCD predictions provide a significantly better
             description of the results than next-to-leading-order QCD
             calculations, unless the latter are matched to a parton
             shower calculation. [Figure not available: see fulltext.] ©
             2014 The Author(s).},
   Doi = {10.1007/JHEP06(2014)112},
   Key = {fds310376}
}

@article{fds350337,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez
             Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Artz,
             S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
             M and Atlay, NB and Atmani, H and Augsten, K and Avolio, G and Avramidou,
             R and Ayoub, MK and Azoulay, AM and Azuelos, G and Bachacou, H and Bachas,
             K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bajic,
             M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura,
             AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
             G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Barsov, S and Bartoldus, R and Bartolini,
             G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bassalat,
             A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool,
             B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
             P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
             A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertram, IA and Bessidskaia Bylund and O and Besson,
             N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya, DS and Bhattarai, P and Bi, R and Bianchi, RM and Biebel,
             O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borecka-Bielska, HM and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
             DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
             G and Brooks, WK and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton,
             CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans,
             R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero,
             J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carter, JWS and Casado, MP and Casha,
             AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Cavaliere, V and Cavallaro, E and Cavalli-Sforza, M and Cavasinni,
             V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen,
             J and Chen, S and Chen, SJ and Chen, X and Chen, Y-H and Cheng, HC and Cheng,
             HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont,
             AR and Chouridou, S and Chow, YS and Chu, MC and Chu, X and Chudoba, J and Chuinard, AJ and Chwastowski, JJ},
   Title = {Measurement of the Lund Jet Plane Using Charged Particles in
             13 TeV Proton-Proton Collisions with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {124},
   Number = {22},
   Pages = {222002},
   Year = {2020},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.124.222002},
   Abstract = {The prevalence of hadronic jets at the LHC requires that a
             deep understanding of jet formation and structure is
             achieved in order to reach the highest levels of
             experimental and theoretical precision. There have been many
             measurements of jet substructure at the LHC and previous
             colliders, but the targeted observables mix physical effects
             from various origins. Based on a recent proposal to
             factorize physical effects, this Letter presents a
             double-differential cross-section measurement of the Lund
             jet plane using 139  fb^{-1} of sqrt[s]=13  TeV
             proton-proton collision data collected with the ATLAS
             detector using jets with transverse momentum above 675 GeV.
             The measurement uses charged particles to achieve a fine
             angular resolution and is corrected for acceptance and
             detector effects. Several parton shower Monte Carlo models
             are compared with the data. No single model is found to be
             in agreement with the measured data across the entire
             plane.},
   Doi = {10.1103/physrevlett.124.222002},
   Key = {fds350337}
}

@article{fds307849,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of the Mass Difference between $t$ and
             $\overline{t}$ Quarks},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {15},
   Pages = {152001},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {April},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.152001},
   Abstract = {We present a direct measurement of the mass difference
             between t and t quarks using tt candidate events in the
             lepton+jets channel, collected with the CDF II detector at
             Fermilab's 1.96 TeV Tevatron pp Collider. We make an event
             by event estimate of the mass difference to construct
             templates for top quark pair signal events and background
             events. The resulting mass difference distribution of data
             is compared to templates of signals and background using a
             maximum likelihood fit. From a sample corresponding to an
             integrated luminosity of 5.6  fb(-1), we measure a mass
             difference, ΔM(top) = M(t) - M(t) = -3.3 ± 1.4(stat) ±
             1.0(syst)  GeV/c2, approximately 2 standard deviations
             away from the CPT hypothesis of zero mass
             difference.},
   Doi = {10.1103/PhysRevLett.106.152001},
   Key = {fds307849}
}

@article{fds307554,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin,
             JF},
   Title = {Measurement of the mass difference between top and anti-top
             quarks in pp collisions at √s=7 TeV using the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {728},
   Pages = {363-379},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.12.010},
   Abstract = {A measurement of the mass difference between top and
             anti-top quarks is presented. In a 4.7 fb−1 data sample of
             proton–proton collisions at s=7 TeV recorded with the
             ATLAS detector at the LHC, events consistent with tt¯
             production and decay into a single charged lepton final
             state are reconstructed. For each event, the mass difference
             between the top and anti-top quark candidate is calculated.
             A two b-tag requirement is used in order to reduce the
             background contribution. A maximum likelihood fit to these
             per-event mass differences yields Δm≡mt−mt¯=0.67±0.61(stat)±0.41(syst)
             GeV, consistent with CPT invariance.},
   Doi = {10.1016/j.physletb.2013.12.010},
   Key = {fds307554}
}

@article{fds307680,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and Barbaro,
             PD and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Canto,
             AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Ramos, JPF and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Garfinkel, AF and Garosi,
             P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and López, OG and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare,
             M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
             JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
             M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
             G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
             A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov,
             A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
             N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Fernández, IR and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov,
             A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, WM and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S},
   Title = {Measurement of the mass difference between top and antitop
             quarks},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {5},
   Pages = {052013},
   Year = {2013},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.052013},
   Abstract = {We present a measurement of the mass difference between top
             (t) and antitop (t̄) quarks using tt̄ candidate events
             reconstructed in the final state with one lepton and
             multiple jets. We use the full data set of Tevatron
             √s=1.96 TeV proton-antiproton collisions recorded by the
             CDF II detector, corresponding to an integrated luminosity
             of 8.7 fb-1. We estimate event by event the mass difference
             to construct templates for top pair signal events and
             background events. The resulting mass difference
             distribution in data compared to signal and background
             templates using a likelihood fit yields ΔMtop=Mt-Mt̄=-1.95±1.11(stat)
             ±0.59(syst) GeV/c2 and is in agreement with the standard
             model prediction of no mass difference. © 2013 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.87.052013},
   Key = {fds307680}
}

@article{fds331626,
   Author = {Collaboration, DAEACDF},
   Title = {Measurement of the mass difference m(D+s)-m(D+) at CDF
             II},
   Journal = {Physical Review},
   Volume = {D68},
   Number = {7},
   Pages = {072004},
   Publisher = {American Physical Society (APS)},
   Year = {2003},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.68.072004},
   Abstract = {We present a measurement of the mass difference
             m(D+s)-m(D+), where both the D+s and D+ are reconstructed in
             the phi pi + decay channel. This measurement uses 11.6 pb-1
             of data collected by CDF II using the new displaced-track
             trigger. The mass difference is found to bem(D+s)-
             m(D+)=99.41±0.38(stat)±0.21(syst) MeV/c2.},
   Doi = {10.1103/PhysRevD.68.072004},
   Key = {fds331626}
}

@article{fds307802,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
             J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli,
             M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi,
             R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
             DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De Barbaro and P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F and D'errico, M and Di Canto,
             A},
   Title = {Measurement of the masses and widths of the bottom baryons
             Σb± and Σb*±},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.092011},
   Abstract = {Using data from pp̄ collisions at √s=1.96TeV recorded by
             the CDF II detector at the Fermilab Tevatron, we present
             improved measurements of the masses and first measurements
             of natural widths of the four bottom baryon resonance states
             Σb+, Σb*+ and Σb-, Σb*-. These states are fully
             reconstructed in their decay modes to Λb0π ± where
             Λb0→Λc+π - with Λc+→pK -π +. The analysis is based
             on a data sample corresponding to an integrated luminosity
             of 6.0fb -1 collected by an online event selection based on
             tracks displaced from the pp̄ interaction point. © 2012
             American Physical Society.},
   Doi = {10.1103/PhysRevD.85.092011},
   Key = {fds307802}
}

@article{fds323243,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
             AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
             JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
             D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko,
             I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
             E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
             C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher,
             F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
             D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
             KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
             PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
             BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
             AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
             SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
             H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Mehta, A and Menzemer,
             S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao,
             T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel,
             R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa,
             T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pitts, KT and Plager, C and Pompoš, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman,
             MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert,
             B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert,
             K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli,
             S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu,
             V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri,
             F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF},
   Title = {Measurement of the moments of the hadronic invariant mass
             distribution in semileptonic B decays},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {5},
   Pages = {1-9},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.051103},
   Abstract = {Using 180 pb -1 of data collected with the CDF II detector
             at the Tevatron, we measure the first two moments of the
             hadronic invariant mass-squared distribution in charmed
             semileptonic B decays. From these we determine the
             nonperturbative Heavy Quark Effective Theory parameters Λ
             and λ 1 used to relate the B meson semileptonic branching
             ratio to the CKM matrix element |V cb|. For a minimum lepton
             momentum of 0.7 GeV/c in the B rest frame we measure the
             first two moments of the D** → D (*)π component to be
             〈m D**2〉 = (5.83 ± 0.16 stat ± 0.08 syst) GeV 2/c 4
             and 〈(m D**2 - 〈m D**2〉) 2〉 = (1.30 ± 0.69 stat ±
             0.22 syst) GeV 4/c 8. Combining these with the discrete mass
             terms from the D and D* mesons, we find the total moments to
             be 〈M Ξc2〉 - m̄ D2 = (0.467 ± 0.038 stat ± 0.068
             syst GeV 2/c 4 and 〈(M Ξc2 - 〈M Ξc2〉) 2〉 = (1.05
             ± 0.26 stat ± 0.13 syst) GeV 4/c 8, where m̄ D is the
             spin-averaged D mass. The systematic error is dominated by
             the uncertainties in the world-average branching ratios used
             to combine the D, D*, and D** contributions. The analysis
             makes no assumptions about the shape or resonant structure
             of the D** → D (*)π invariant mass distribution. © 2005
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.71.051103},
   Key = {fds323243}
}

@article{fds310390,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Bessner, M and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Measurement of the muon reconstruction performance of the
             ATLAS detector using 2011 and 2012 LHC proton-proton
             collision data.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {11},
   Pages = {3130},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3130-x},
   Abstract = {This paper presents the performance of the ATLAS muon
             reconstruction during the LHC run with [Formula: see text]
             collisions at [Formula: see text]-8 TeV in 2011-2012,
             focusing mainly on data collected in 2012. Measurements of
             the reconstruction efficiency and of the momentum scale and
             resolution, based on large reference samples of [Formula:
             see text], [Formula: see text] and [Formula: see text]
             decays, are presented and compared to Monte Carlo
             simulations. Corrections to the simulation, to be used in
             physics analysis, are provided. Over most of the covered
             phase space (muon [Formula: see text] and [Formula: see
             text] GeV) the efficiency is above [Formula: see text] and
             is measured with per-mille precision. The momentum
             resolution ranges from [Formula: see text] at central
             rapidity and for transverse momentum [Formula: see
             text] GeV, to [Formula: see text] at large rapidity and
             [Formula: see text] GeV. The momentum scale is known with
             an uncertainty of [Formula: see text] to [Formula: see text]
             depending on rapidity. A method for the recovery of final
             state radiation from the muons is also presented.},
   Doi = {10.1140/epjc/s10052-014-3130-x},
   Key = {fds310390}
}

@article{fds347445,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Measurement of the nuclear modification factor for inclusive
             jets in Pb+Pb collisions at √sNN=5.02 TeV with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {790},
   Pages = {108-128},
   Year = {2019},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.10.076},
   Abstract = {Measurements of the yield and nuclear modification factor,
             RAA, for inclusive jet production are performed using 0.49
             nb−1 of Pb+Pb data at sNN=5.02TeV and 25 pb−1 of Pb+Pb
             data at s=5.02TeV with the ATLAS detector at the LHC. Jets
             are reconstructed with the anti-kt algorithm with radius
             parameter R=0.4 and are measured over the transverse
             momentum range of 40–1000 GeV in six rapidity intervals
             covering |y|<2.8. The magnitude of RAA increases with
             increasing jet transverse momentum, reaching a value of
             approximately 0.6 at 1 TeV in the most central collisions.
             The magnitude of RAA also increases towards peripheral
             collisions. The value of RAA is independent of rapidity at
             low jet transverse momenta, but it is observed to decrease
             with increasing rapidity at high transverse
             momenta.},
   Doi = {10.1016/j.physletb.2018.10.076},
   Key = {fds347445}
}

@article{fds371118,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
             CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
             P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
             C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev,
             V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
             JF},
   Title = {Measurement of the nuclear modification factor of b-jets in
             5.02 TeV Pb+Pb collisions with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {5},
   Year = {2023},
   Month = {May},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11427-9},
   Abstract = {This paper presents a measurement of b-jet production in
             Pb+Pb and pp collisions at sNN=5.02 TeV with the ATLAS
             detector at the LHC. The measurement uses 260 pb - 1 of pp
             collisions collected in 2017 and 1.4 nb - 1 of Pb+Pb
             collisions collected in 2018. In both collision systems,
             jets are reconstructed via the anti- kt algorithm. The
             b-jets are identified from a sample of jets containing muons
             from the semileptonic decay of b-quarks using template fits
             of the muon momentum relative to the jet axis. In pp
             collisions, b-jets are reconstructed for radius parameters
             R= 0.2 and R= 0.4 , and only R= 0.2 jets are used in Pb+Pb
             collisions. For comparison, inclusive R= 0.2 jets are also
             measured using 1.7 nb - 1 of Pb+Pb collisions collected in
             2018 and the same pp collision data as the b-jet
             measurement. The nuclear modification factor, RAA , is
             calculated for both b-jets and inclusive jets with R= 0.2
             over the transverse momentum range of 80–290 GeV. The
             nuclear modification factor for b-jets decreases from
             peripheral to central collisions. The ratio of the b-jet RAA
             to inclusive jet RAA is also presented and suggests that the
             RAA for b-jets is larger than that for inclusive jets in
             central Pb+Pb collisions. The measurements are compared with
             theoretical calculations and suggest a role for mass and
             colour-charge effects in partonic energy loss in heavy-ion
             collisions.},
   Doi = {10.1140/epjc/s10052-023-11427-9},
   Key = {fds371118}
}

@article{fds307538,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O},
   Title = {Measurement of the parity-violating asymmetry parameter αb
             and the helicity amplitudes for the decay Λb0 →j /ψ Λ0
             with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.092009},
   Abstract = {A measurement of the parity-violating decay asymmetry
             parameter, αb, and the helicity amplitudes for the decay
             Λb0→J/ψ(μ+μ-)Λ0(pπ-) is reported. The analysis is
             based on 1400 Λb0 and Λ¯b0 baryons selected in 4.6 fb-1
             of proton-proton collision data with a center-of-mass energy
             of 7 TeV recorded by the ATLAS experiment at the LHC. By
             combining the Λb0 and Λ¯b0 samples under the assumption
             of CP conservation, the value of αb is measured to be
             0.30±0.16(stat)±0.06(syst). This measurement provides a
             test of theoretical models based on perturbative QCD or
             heavy-quark effective theory.},
   Doi = {10.1103/PhysRevD.89.092009},
   Key = {fds307538}
}

@article{fds356618,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos, SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Pozo, JAA and Aperio Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz, V and Araujo Pereira, R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {Measurement of the photon identification efficiencies with
             the ATLAS detector using LHC Run 2 data collected in 2015
             and 2016},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {3},
   Year = {2019},
   Month = {March},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-6650-6},
   Abstract = {The efficiency of the photon identification criteria in the
             ATLAS detector is measured using 36.1fb1 to 36.7fb1 of pp
             collision data at s=13 TeV collected in 2015 and 2016. The
             efficiencies are measured separately for converted and
             unconverted isolated photons, in four different
             pseudorapidity regions, for transverse momenta between 10
             GeV and 1.5 TeV. The results from the combination of three
             data-driven techniques are compared with the predictions
             from simulation after correcting the variables describing
             the shape of electromagnetic showers in simulation for the
             average differences observed relative to data.
             Data-to-simulation efficiency ratios are determined to
             account for the small residual efficiency differences. These
             factors are measured with uncertainties between 0.5% and 5%
             depending on the photon transverse momentum and
             pseudorapidity. The impact of the isolation criteria on the
             photon identification efficiency, and that of additional
             soft pp interactions, are also discussed. The probability of
             reconstructing an electron as a photon candidate is measured
             in data, and compared with the predictions from simulation.
             The efficiency of the reconstruction of photon conversions
             is measured using a sample of photon candidates from Z→
             μμγ events, exploiting the properties of the ratio of the
             energies deposited in the first and second longitudinal
             layers of the ATLAS electromagnetic calorimeter.},
   Doi = {10.1140/epjc/s10052-019-6650-6},
   Key = {fds356618}
}

@article{fds322003,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
             N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
             F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
             EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
             R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo,
             F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez,
             VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El Moursli and RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Measurement of the photon identification efficiencies with
             the ATLAS detector using LHC Run-1 data.},
   Journal = {Eur Phys J C Part Fields},
   Volume = {76},
   Number = {12},
   Pages = {666},
   Year = {2016},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4507-9},
   Abstract = {The algorithms used by the ATLAS Collaboration to
             reconstruct and identify prompt photons are described.
             Measurements of the photon identification efficiencies are
             reported, using 4.9 fb[Formula: see text] of pp collision
             data collected at the LHC at [Formula: see text] [Formula:
             see text] and 20.3 fb[Formula: see text] at [Formula: see
             text] [Formula: see text]. The efficiencies are measured
             separately for converted and unconverted photons, in four
             different pseudorapidity regions, for transverse momenta
             between 10 [Formula: see text] and 1.5 [Formula: see
             text]. The results from the combination of three data-driven
             techniques are compared to the predictions from a simulation
             of the detector response, after correcting the
             electromagnetic shower momenta in the simulation for the
             average differences observed with respect to data.
             Data-to-simulation efficiency ratios used as correction
             factors in physics measurements are determined to account
             for the small residual efficiency differences. These factors
             are measured with uncertainties between 0.5% and 10% in
             7 [Formula: see text] data and between 0.5% and 5.6% in
             8 [Formula: see text] data, depending on the photon
             transverse momentum and pseudorapidity.},
   Doi = {10.1140/epjc/s10052-016-4507-9},
   Key = {fds322003}
}

@article{fds372121,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
             A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport, PP and Aloisio,
             A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez
             Fernandez, A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
             Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
             V and Arcangeletti, C and Arce, ATH},
   Title = {Measurement of the polarisation of W bosons produced in
             top-quark decays using dilepton events at s=13 TeV with the
             ATLAS experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {843},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.137829},
   Abstract = {A measurement of the polarisation of W bosons produced in
             top-quark decays is presented, using proton–proton
             collision data at a centre-of-mass energy of s=13 TeV. The
             data were collected by the ATLAS detector at the Large
             Hadron Collider and correspond to an integrated luminosity
             of 139 fb−1. The measurement is performed selecting tt¯
             events decaying into final states with two charged leptons
             (electrons or muons) and at least two b-tagged jets. The
             polarisation is extracted from the differential
             cross-section distribution of the cos⁡θ⁎ variable,
             where θ⁎ is the angle between the momentum direction of
             the charged lepton from the W boson decay and the reversed
             momentum direction of the b-quark from the top-quark decay,
             both calculated in the W boson rest frame. Parton-level
             results, corrected for the detector acceptance and
             resolution, are presented for the cos⁡θ⁎ angle. The
             measured fractions of longitudinal, left- and right-handed
             polarisation states are found to be f0=0.684±0.005(stat.)±0.014(syst.),
             fL=0.318±0.003(stat.)±0.008(syst.) and
             fR=−0.002±0.002(stat.)±0.014(syst.), in agreement with
             the Standard Model prediction.},
   Doi = {10.1016/j.physletb.2023.137829},
   Key = {fds372121}
}

@article{fds307725,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the polarisation of W bosons produced with
             large transverse momentum in pp collisions at √s =7 TeV
             with the ATLAS experiment},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {5},
   Pages = {1-30},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2001-6},
   Abstract = {This paper describes an analysis of the angular distribution
             of W→eν and W→μν decays, using data from pp
             collisions at √s =7 TeV recorded with the ATLAS detector
             at the LHC in 2010, corresponding to an integrated
             luminosity of about 35 pb-1. Using the decay lepton
             transverse momentum and the missing transverse momentum, the
             W decay angular distribution projected onto the transverse
             plane is obtained and analysed in terms of helicity
             fractions f0, fL and fR over two ranges of W transverse
             momentum (pWT): 35 < pWT < 50 GeV and pWT > 50 GeV. Good
             agreement is found with theoretical predictions. For pWT >50
             GeV, the values of f0 and fL-fR, averaged over charge and
             lepton flavour, are measured to be: f0=0. 127±0. 030±0.
             108 and fL-fR=0. 252±0. 017±0. 030, where the first
             uncertainties are statistical, and the second include all
             systematic effects. © 2012 CERN for the benefit of the
             ATLAS collaboration.},
   Doi = {10.1140/epjc/s10052-012-2001-6},
   Key = {fds307725}
}

@article{fds310282,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Measurement of the production and differential cross
             sections of W+W- bosons in association
             with jets in pp¯ collisions at √s = 1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.111101},
   Abstract = {We present a measurement of the W-boson-pair production
             cross section in pp¯ collisions at 1.96 TeV center-of-mass
             energy and the first measurement of the differential cross
             section as a function of jet multiplicity and leading-jet
             energy. The W+W- cross section is measured in the final
             state comprising two charged leptons and neutrinos, where
             either charged lepton can be an electron or a muon. Using
             data collected by the CDF experiment corresponding to
             9.7fb-1 of integrated luminosity, a total of 3027 collision
             events consistent with W+W- production are observed with an
             estimated background contribution of 1790 ± 190 events. The
             measured total cross section is σ(pp¯ → W+W-)= 14.0 ±
             0.6 (stat)-1.0+1.2 (syst) ± 0.8 (lumi) pb, consistent with
             the standard model prediction.},
   Doi = {10.1103/PhysRevD.91.111101},
   Key = {fds310282}
}

@article{fds356561,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V},
   Title = {Measurement of the production cross section for a Higgs
             boson in association with a vector boson in the
             H → WW → ℓνℓν channel in pp
             collisions at s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {798},
   Year = {2019},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.134949},
   Abstract = {A measurement of the Higgs boson production cross sections
             via associated WH and ZH production using
             H→WW⁎→ℓνℓν decays, where ℓ stands for either
             an electron or a muon, is presented. Results for combined WH
             and ZH production are also presented. The analysis uses
             events produced in proton–proton collisions collected with
             the ATLAS detector at the Large Hadron Collider in 2015 and
             2016. The data correspond to an integrated luminosity of
             36.1fb−1 recorded at a centre-of-mass energy of 13 TeV.
             The products of the H→WW⁎ branching fraction times the
             WH and ZH cross sections are measured to be
             0.67−0.27+0.31(stat.)−0.14+0.18(syst.) pb and
             0.54−0.24+0.31(stat.)−0.07+0.15(syst.) pb respectively,
             in agreement with the Standard Model predictions.},
   Doi = {10.1016/j.physletb.2019.134949},
   Key = {fds356561}
}

@article{fds307757,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the production cross section for Z/γ* in
             association with jets in pp collisions at √s=7TeV with the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.032009},
   Abstract = {Results are presented on the production of jets of particles
             in association with a Z/γ* boson, in proton-proton
             collisions at √s=7TeV with the ATLAS detector. The
             analysis includes the full 2010 data set, collected with a
             low rate of multiple proton-proton collisions in the
             accelerator, corresponding to an integrated luminosity of
             36pb-1. Inclusive jet cross sections in Z/γ* events, with
             Z/γ* decaying into electron or muon pairs, are measured for
             jets with transverse momentum pT>30GeV and jet rapidity
             |y|<4.4. The measurements are compared to
             next-to-leading-order perturbative QCD calculations, and to
             predictions from different Monte Carlo generators
             implementing leading-order matrix elements supplemented by
             parton showers. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.85.032009},
   Key = {fds307757}
}

@article{fds307736,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the production cross section of an isolated
             photon associated with jets in proton-proton collisions at
             √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.092014},
   Abstract = {A measurement of the cross section for the production of an
             isolated photon in association with jets in proton-proton
             collisions at a center-of-mass energy √s=7TeV is
             presented. Photons are reconstructed in the pseudorapidity
             range |ηγ|<1.37 and with a transverse energy ETγ>25GeV.
             Jets are reconstructed in the rapidity range |yjet|<4.4 and
             with a transverse momentum pTjet>20GeV. The differential
             cross section dσ/dETγ is measured, as a function of the
             photon transverse energy, for three different rapidity
             ranges of the leading-pT jet: |yjet|<1.2, 1.2≤|yjet|<2.8
             and 2.8≤|yjet|<4.4. For each rapidity configuration the
             same-sign (ηγyjet 0) and opposite-sign (ηγyjet<0) cases
             are studied separately. The results are based on an
             integrated luminosity of 37pb-1, collected with the ATLAS
             detector at the LHC. Next-to-leading order perturbative QCD
             calculations are found to be in fair agreement with the
             data, except for ETγ 45GeV, where the theoretical
             predictions overestimate the measured cross sections. ©
             2012 CERN.},
   Doi = {10.1103/PhysRevD.85.092014},
   Key = {fds307736}
}

@article{fds307650,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E and Arik, M and Armbruster, AJ},
   Title = {Measurement of the production cross section of jets in
             association with a Z boson in pp collisions at √s=7 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {7},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP07(2013)032},
   Abstract = {Measurements of the production of jets of particles in
             association with a Z boson in pp collisions at √s=7 TeV
             are presented, using data corresponding to an integrated
             luminosity of 4.6 fb-1 collected by the ATLAS experiment at
             the Large Hadron Collider. Inclusive and differential jet
             cross sections in Z events, with Z decaying into electron or
             muon pairs, are measured for jets with transverse momentum p
             T > 30 GeV and rapidity |y| < 4.4. The results are compared
             to next-to-leading-order perturbative QCD calculations, and
             to predictions from different Monte Carlo generators based
             on leading-order and next-to-leading-order matrix elements
             supplemented by parton showers. [Figure not available: see
             fulltext.] © 2013 CERN for the benefit of the ATLAS
             collaboration.},
   Doi = {10.1007/JHEP07(2013)032},
   Key = {fds307650}
}

@article{fds360567,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala,
             J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada
             Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
             M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
             JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
             V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S},
   Title = {Measurement of the production cross section of pairs of
             isolated photons in pp collisions at 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {11},
   Year = {2021},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2021)169},
   Abstract = {A measurement of prompt photon-pair production in
             proton-proton collisions at s = 13 TeV is presented. The
             data were recorded by the ATLAS detector at the LHC with an
             integrated luminosity of 139 fb−1. Events with two photons
             in the well-instrumented region of the detector are
             selected. The photons are required to be isolated and have a
             transverse momentum of pT,γ1(2)> 40 (30) GeV for the
             leading (sub-leading) photon. The differential cross
             sections as functions of several observables for the
             diphoton system are measured and compared with theoretical
             predictions from state-of-the-art Monte Carlo and
             fixed-order calculations. The QCD predictions from
             next-to-next-to-leading-order calculations and multi-leg
             merged calculations are able to describe the measured
             integrated and differential cross sections within
             uncertainties, whereas lower-order calculations show
             significant deviations, demonstrating that higher-order
             perturbative QCD corrections are crucial for this process.
             The resummed predictions with parton showers additionally
             provide an excellent description of the low
             transverse-momentum regime of the diphoton system. [Figure
             not available: see fulltext.].},
   Doi = {10.1007/JHEP11(2021)169},
   Key = {fds360567}
}

@article{fds307544,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
             M},
   Title = {Measurement of the production cross section of prompt J/ψ
             mesons in association with a W± boson in pp collisions at
             √s = 7 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {4},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2014)172},
   Abstract = {The process pp → W±J/ψ provides a powerful probe of the
             production mechanism of charmonium in hadronic collisions,
             and is also sensitive to multiple parton interactions in the
             colliding protons. Using the 2011 ATLAS dataset of 4.5 fb-1
             of p s = 7TeV pp collisions at the LHC, the first
             observation is made of the production of W± + prompt J/
             events in hadronic collisions, using W± → μ and J/ψ →
             μ+μ-. A yield of 27.4±7.5 -6.5 W± + prompt J/ψ events
             is observed, with a statistical significance of 5.1. The
             production rate as a ratio to the inclusive W± boson
             production rate is measured, and the double parton
             scattering contribution to the cross section is estimated.
             Copyright CERN, for the benefit of the ATLAS
             Collaboration.},
   Doi = {10.1007/JHEP04(2014)172},
   Key = {fds307544}
}

@article{fds356678,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza,
             A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli, M and Antonov,
             A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A},
   Title = {Measurement of the production cross section of three
             isolated photons in pp collisions at √s=8 TeV using the
             ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {781},
   Pages = {55-76},
   Year = {2018},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.03.057},
   Abstract = {A measurement of the production of three isolated photons in
             proton–proton collisions at a centre-of-mass energy s=8
             TeV is reported. The results are based on an integrated
             luminosity of 20.2 fb−1 collected with the ATLAS detector
             at the LHC. The differential cross sections are measured as
             functions of the transverse energy of each photon, the
             difference in azimuthal angle and in pseudorapidity between
             pairs of photons, the invariant mass of pairs of photons,
             and the invariant mass of the triphoton system. A
             measurement of the inclusive fiducial cross section is also
             reported. Next-to-leading-order perturbative QCD predictions
             are compared to the cross-section measurements. The
             predictions underestimate the measurement of the inclusive
             fiducial cross section and the differential measurements at
             low photon transverse energies and invariant masses. They
             provide adequate descriptions of the measurements at high
             values of the photon transverse energies, invariant mass of
             pairs of photons, and invariant mass of the triphoton
             system.},
   Doi = {10.1016/j.physletb.2018.03.057},
   Key = {fds356678}
}

@article{fds316847,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of the production cross-section of a single top
             quark in association with a W boson at 8 TeV with the ATLAS
             experiment},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {1},
   Pages = {1-48},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2016)064},
   Abstract = {The cross-section for the production of a single top quark
             in association with a W boson in proton-proton collisions at
             √s = 8TeV is measured. The dataset corresponds to an
             integrated luminosity of 20.3 fb−1, collected by the ATLAS
             detector in 2012 at the Large Hadron Collider at CERN.
             Events containing two leptons and one central b-jet are
             selected. The W t signal is separated from the backgrounds
             using boosted decision trees, each of which combines a
             number of discriminating variables into one classifier.
             Production of W t events is observed with a significance of
             7.7σ. The cross-section is extracted in a profile
             likelihood fit to the classifier output distributions. The W
             t cross-section, inclusive of decay modes, is measured to be
             23.0 ± 1.3(stat.)− 3.5+ 3.2(syst.)±1.1(lumi.) pb. The
             measured cross-section is used to extract a value for the
             CKM matrix element |Vtb| of 1.01 ± 0.10 and a lower limit
             of 0.80 at the 95% confidence level. The cross-section for
             the production of a top quark and a W boson is also measured
             in a fiducial acceptance requiring two leptons with pT> 25
             GeV and |η| < 2.5, one jet with pT> 20 GeV and |η| < 2.5,
             and ETmiss > 20 GeV, including both W t and top-quark pair
             events as signal. The measured value of the fiducial
             cross-section is 0.85 ± 0.01(stat.)− 0.07+
             0.07(syst.)±0.03(lumi.) pb.},
   Doi = {10.1007/JHEP01(2016)064},
   Key = {fds316847}
}

@article{fds356683,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Measurement of the production cross-section of a single top
             quark in association with a Z boson in proton–proton
             collisions at 13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {780},
   Pages = {557-577},
   Year = {2018},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.03.023},
   Abstract = {The production of a top quark in association with a Z boson
             is investigated. The proton–proton collision data
             collected by the ATLAS experiment at the LHC in 2015 and
             2016 at a centre-of-mass energy of s=13TeV are used,
             corresponding to an integrated luminosity of 36.1fb−1.
             Events containing three identified leptons (electrons and/or
             muons) and two jets, one of which is identified as a b-quark
             jet are selected. The major backgrounds are diboson, tt¯
             and Z+jets production. A neural network is used to improve
             the background rejection and extract the signal. The
             resulting significance is 4.2σ in the data and the expected
             significance is 5.4σ. The measured cross-section for tZq
             production is 600±170(stat.)±140(syst.)fb.},
   Doi = {10.1016/j.physletb.2018.03.023},
   Key = {fds356683}
}

@article{fds376247,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Bourdarios, CA and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
             SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
             CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
   Title = {Measurement of the production cross-section of J/ψ and
             ψ(2S) mesons in pp collisions at s=13 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {84},
   Number = {2},
   Year = {2024},
   Month = {February},
   url = {http://dx.doi.org/10.1140/epjc/s10052-024-12439-9},
   Abstract = {Measurements of the differential production cross-sections
             of prompt and non-prompt J/ψ and ψ(2S) mesons with
             transverse momenta between 8 and 360 GeV and rapidity in
             the range |y|<2 are reported. Furthermore, measurements of
             the non-prompt fractions of J/ψ and ψ(2S), and the prompt
             and non-prompt ψ(2S)-to-J/ψ production ratios, are
             presented. The analysis is performed using 140 fb-1 of
             s=13 TeV pp collision data recorded by the ATLAS detector
             at the LHC during the years 2015–2018.},
   Doi = {10.1140/epjc/s10052-024-12439-9},
   Key = {fds376247}
}

@article{fds310381,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik,
             M},
   Title = {Measurement of the production of a W boson in association
             with a charm quark in pp collisions at √s = 7TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {5},
   Pages = {1-67},
   Publisher = {Springer-Verlag},
   Year = {2014},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2014)068},
   Abstract = {The production of a W boson in association with a single
             charm quark is studied using 4.6 fb-1 of pp collision data
             at √s = 7TeV collected with the ATLAS detector at the
             Large Hadron Collider. In events in which a W boson decays
             to an electron or muon, the charm quark is tagged either by
             its semileptonic decay to a muon or by the presence of a
             charmed meson. The integrated and differential cross
             sections as a function of the pseudorapidity of the lepton
             from the W-boson decay are measured. Results are compared to
             the predictions of next-to-leading-order QCD calculations
             obtained from various parton distribution function
             parameterisations. The ratio of the strange-to-down
             sea-quark distributions is determined to be 0.96+-00.30 at
             Q2 = 1.9 GeV, which supports the hypothesis of an
             SU(3)-symmetric composition of the light-quark sea.
             Additionally the cross-section ratio σ(W+ + c)/σ(W- +c) is
             compared to the predictions obtained using parton
             distribution function parameterisations with different
             assumptions about the s–s quark asymmetry.},
   Doi = {10.1007/JHEP05(2014)068},
   Key = {fds310381}
}

@article{fds373466,
   Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben,
             M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori, G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang, R and Zhang, J and Berlendis,
             S and Cheu, E and Cui, Z and Ghosh, A and Johns, KA and Lampl, W and Lindley,
             RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou,
             H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai,
             G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Tost, M and Unal, M and Huseynov, N},
   Title = {Measurement of the production of a W boson in association
             with a charmed hadron in pp collisions at √s=13 TeV with
             the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {108},
   Number = {3},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.108.032012},
   Abstract = {The production of a W boson in association with a single
             charm quark is studied using 140 fb - 1 of s = 13 TeV
             proton-proton collision data collected with the ATLAS
             detector at the Large Hadron Collider. The charm quark is
             tagged by the presence of a charmed hadron reconstructed
             with a secondary-vertex fit. The W boson is reconstructed
             from the decay to either an electron or a muon and the
             missing transverse momentum present in the event. The
             charmed mesons reconstructed are D + → K - π + π + and D
             * + → D 0 π + → ( K - π + ) π + and the charge
             conjugate decays in the fiducial regions where p T ( e , μ
             ) > 30 GeV , | η ( e , μ ) | < 2.5 , p T ( D ( * ) ) > 8
             GeV , and | η ( D ( * ) ) | < 2.2 . The integrated and
             normalized differential cross sections as a function of the
             pseudorapidity of the lepton from the W boson decay, and of
             the transverse momentum of the charmed hadron, are extracted
             from the data using a profile likelihood fit. The measured
             total fiducial cross sections are σ fid OS - SS ( W - + D +
             ) = 50.2 ± 0.2 ( stat ) - 2.3 + 2.4 ( syst ) pb , σ fid OS
             - SS ( W + + D - ) = 48.5 ± 0.2 ( stat ) - 2.2 + 2.3 ( syst
             ) pb , σ fid OS - SS ( W - + D * + ) = 51.1 ± 0.4 ( stat )
             - 1.8 + 1.9 ( syst ) pb , and σ fid OS - SS ( W + + D * - )
             = 50.0 ± 0.4 ( stat ) - 1.8 + 1.9 ( syst ) pb . Results are
             compared with the predictions of next-to-leading-order
             quantum chromodynamics calculations performed using
             state-of-the-art parton distribution functions.
             Additionally, the ratio of charm to anticharm production
             cross sections is studied to probe the s - s ¯ quark
             asymmetry. The ratio is found to be R c ± = 0.971 ± 0.006
             ( stat ) ± 0.011 ( syst ) . The ratio and cross-section
             measurements are consistent with the predictions obtained
             with parton distribution function sets that have a symmetric
             s - s ¯ sea, indicating that any s - s ¯ asymmetry in the
             Bjorken- x region relevant for this measurement is
             small.},
   Doi = {10.1103/PhysRevD.108.032012},
   Key = {fds373466}
}

@article{fds307768,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R and Ask, S},
   Title = {Measurement of the pseudorapidity and transverse momentum
             dependence of the elliptic flow of charged particles in
             lead-lead collisions at sNN=2.76 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {707},
   Number = {3-4},
   Pages = {330-348},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.12.056},
   Abstract = {This Letter describes the measurement of elliptic flow of
             charged particles in lead-lead collisions at sNN=2.76 TeV
             using the ATLAS detector at the Large Hadron Collider (LHC).
             The results are based on an integrated luminosity of
             approximately 7 μb-1. Elliptic flow is measured over a wide
             region in pseudorapidity, |η|<2.5, and over a broad range
             in transverse momentum, 0.5<pT<20 GeV. The elliptic flow
             parameter v2 is obtained by correlating individual tracks
             with the event plane measured using energy deposited in the
             forward calorimeters. As a function of transverse momentum,
             v2(pT) reaches a maximum at pT of about 3 GeV, then
             decreases and becomes weakly dependent on pT above 7-8 GeV.
             Over the measured pseudorapidity region, v2 is found to be
             only weakly dependent on η, with less variation than
             observed at lower beam energies. The results are discussed
             in the context of previous measurements at lower collision
             energies, as well as recent results from the LHC. © 2011
             CERN.},
   Doi = {10.1016/j.physletb.2011.12.056},
   Key = {fds307768}
}

@article{fds308000,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
             M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
             MA},
   Title = {Measurement of the ratio of branching fractions B(B±→J/
             ψπ±)/B(B±→J/ψK±)},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.112003},
   Abstract = {We report a measurement of the ratio of branching fractions
             of the decays B±→J/ψπ± and B±→J/ψK± using the CDF
             II detector at the Fermilab Tevatron Collider. The signal
             from the Cabbibo-suppressed B±→J/ψπ± decay is
             separated from B±→J/ψK± using the B±→J/ψK±
             invariant mass distribution and the kinematical differences
             of the hadron track in the two decay modes. From a sample of
             220pb-1 of pp̄ collisions at s=1.96TeV, we observe 91±15
             B±→J/ψπ± events together with 1883±34 B±→J/ψK±
             events. The ratio of branching fractions is found to be
             B(B±→J/ψπ±)/ B(B±→J/ψK±)=(4.86±0.82(stat)±0.15(syst))%.
             © 2009 The American Physical Society.},
   Doi = {10.1103/PhysRevD.79.112003},
   Key = {fds308000}
}

@article{fds308122,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro,
             A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cresciolo, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
             PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and DiTuro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo,
             T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
             JP and Field, R and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
             I and Gallinaro, M and Galyardt, J and Garcia, JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris,
             N and Giolo, K and Giordani, M and Giromini, P and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare,
             M and Harper, S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser,
             J and Hays, C and Heijboer, A and Heinemann, B and Heinrich, J and Herndon,
             M and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
             A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karchin, PE and Kato,
             Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
             J and Lysak, R and Lytken, E and MacK, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty,
             R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian,
             C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Ogawa, T and Oh, SH and Oh,
             YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
             G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn,
             F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton,
             P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
             A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Sjolin,
             J},
   Title = {Measurement of the ratio of branching fractions
             B(D0→K+π-)/ B(D0→K-π+) using the CDF II
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {74},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.74.031109},
   Abstract = {We present a measurement of RB, the ratio of the branching
             fraction for the rare decay D0→K+π- to that for the
             Cabibbo-favored decay D0→K-π+. Charge-conjugate decays
             are implicitly included. A signal of 2005±104 events for
             the decay D0→K+π- is obtained using the CDF II detector
             at the Fermilab Tevatron collider. The data set corresponds
             to an integrated luminosity of 0.35fb-1 produced in p̄p
             collisions at s=1.96TeV. Assuming no mixing, we find
             RB=[4.05±0.21(stat)±0.11(syst)] ×10-3. This measurement
             is consistent with the world average, and comparable in
             accuracy with the best measurements from other experiments.
             © 2006 The American Physical Society.},
   Doi = {10.1103/PhysRevD.74.031109},
   Key = {fds308122}
}

@article{fds356613,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger,
             M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou,
             C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Arduh, FA and Arguin, JF},
   Title = {Measurement of the ratio of cross sections for inclusive
             isolated-photon production in pp collisions at √s = 13 and
             8 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {4},
   Year = {2019},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2019)093},
   Abstract = {The ratio of the cross sections for inclusive
             isolated-photon production in pp collisions at
             centre-of-mass energies of 13 and 8 TeV is measured using
             the ATLAS detector at the LHC. The integrated luminosities
             of the 13 TeV and 8 TeV datasets are 3.2 fb −1 and 20.2 fb
             −1 , respectively. The ratio is measured as a function of
             the photon transverse energy in different regions of the
             photon pseudorapidity. The predictions from
             next-to-leading-order perturbative QCD calculations are
             compared with the measured ratio. The experimental
             systematic uncertainties as well as the uncertainties
             affecting the predictions are evaluated taking into account
             the correlations between the two centre-of-mass energies,
             resulting in a reduction of up to a factor of 2.5 (5) in the
             experimental (theoretical) systematic uncertainties. The
             predictions based on several parameterisations of the proton
             parton distribution functions agree with the data within the
             reduced experimental and theoretical uncertainties. In
             addition, this ratio to that of the fiducial cross sections
             for Z boson production at 13 and 8 TeV using the decay
             channels Z → e + e − and Z → μ + μ − is made and
             compared with the theoretical predictions. In this double
             ratio, a further reduction of the experimental uncertainty
             is obtained because the uncertainties arising from the
             luminosity measurement cancel out. The predictions describe
             the measurements of the double ratio within the theoretical
             and experimental uncertainties.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP04(2019)093},
   Key = {fds356613}
}

@article{fds308184,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin,
             B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto,
             J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette,
             F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar,
             V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
             F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR},
   Title = {Measurement of the ratio of differential cross sections for
             W and Z boson production as a function of transverse
             momentum in pp̄ collisions at √s = 1.8
             TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {517},
   Number = {3-4},
   Pages = {299-308},
   Publisher = {Elsevier BV},
   Year = {2001},
   Month = {October},
   url = {http://dx.doi.org/10.1016/S0370-2693(01)01020-6},
   Abstract = {We report on a measurement of the ratio of the differential
             cross sections for W and Z boson production as a function of
             transverse momentum in proton-antiproton collisions at √s
             = 1.8 TeV. This measurement uses data recorded by the DØ
             detector at the Fermilab Tevatron in 1994-1995. It
             represents the first investigation of a proposal that ratios
             between W and Z observables can be calculated reliably using
             perturbative QCD, even when the individual observables are
             not. Using the ratio of differential cross sections reduces
             both experimental and theoretical uncertainties, and can
             therefore provide smaller overall uncertainties in the
             measured mass and width of the W boson than current methods
             used at hadron colliders. © 2001 Elsevier Science B.V. All
             rights reserved.},
   Doi = {10.1016/S0370-2693(01)01020-6},
   Key = {fds308184}
}

@article{fds308081,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Casarsa, M and Castro,
             A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Cyr, D and Daronco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart,
             D and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza,
             BD and Dittmann, JR and Dituro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher,
             R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
             JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster,
             GW and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay,
             C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson,
             A and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths,
             M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
             RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
             A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
             S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee,
             SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
             D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
             P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino,
             C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
             M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt,
             J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman,
             J and Nagano, A and Naganoma, J and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
             A and Ranjan, N and Rappoccio, S and Reisert, B and Rekovic, V and Renton,
             P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Sjolin, J and Slaughter,
             AJ},
   Title = {Measurement of the ratios of branching fractions B(Bs0→Ds-
             π+π+π-)/B(B0→D-π+π+π-) and B(Bs0→Ds-π+)/
             B(B0→D-π+)},
   Journal = {Physical Review Letters},
   Volume = {98},
   Number = {6},
   Pages = {061802},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.98.061802},
   Abstract = {Using 355pb-1 of data collected by the CDF II detector in
             pp̄ collisions at s=1.96TeV at the Fermilab Tevatron, we
             study the fully reconstructed hadronic decays
             B(s)0→D(s)-π+ and B(s)0→D(s)- π+π+π-. We present the
             first measurement of the ratio of branching fractions
             B(Bs0→Ds-π+π+π-)/B(B0→D-π+π+π-)=1.
             05±0.10(stat)±0.22(syst). We also update our measurement
             of B(Bs0→Ds-π+)/B(B0→D-π+) to 1.13±0.08(stat)±0.
             23(syst), improving the statistical uncertainty by more than
             a factor of 2. We find B(Bs0→Ds-π+)=[3.8±0.3(stat)±1.3(syst)]×10-3
             and B(Bs0→Ds-π+π+π-)=[8.4±0.8(stat)±3.2(syst)]
             ×10-3. © 2007 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.98.061802},
   Key = {fds308081}
}

@article{fds361223,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
             J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
             J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Connolly, A and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cruz, A and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'onofrio, M and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, J and DiTuro, P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers,
             J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
             M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
             LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia, JE and Sciverez, MG and Garfinkel, AF and Gay,
             C and Gerberich, H and Gerchtein, E and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski,
             D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
             M and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Costa, JGD and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper,
             S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heijboer, A and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karagoz-Unel, M and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute,
             M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreps, M and Kreymer, A and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
             H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, P and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
             A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman,
             R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Papikonomou, A and Paramonov,
             AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, K and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton,
             P and Rescigno, M and Richter, S and Rimondi, F and Rinnert, K and Ristori,
             L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli,
             S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Salto, O and Saltzberg, D and Sanchez,
             C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro,
             A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
             A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro,
             MD},
   Title = {Measurement of the ratios of branching fractions
             B(Bs0→Ds-π+)/ B(B0→D-π+) and B(B+→D̄0π+)/B(B0→D-π+)},
   Journal = {Physical Review Letters},
   Volume = {96},
   Number = {19},
   Pages = {191801},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevLett.96.191801},
   Abstract = {We report an observation of the decay Bs0→Ds-π+ in pp̄
             collisions at s=1.96TeV using 115pb-1 of data collected by
             the CDF II detector at the Fermilab Tevatron. We observe
             83±11(stat) Bs0→Ds-π+ candidates, representing a large
             increase in statistics over previous measurements and the
             first observation of this decay at a pp̄ collider. We
             present the first measurement of the relative branching
             fraction B(Bs0→Ds-π+)/B(B0→D-π+)=1.32±0.18(stat)±0.38(syst)
             . We also measure B(B+→D̄0π+)/B(B0→D-π+)=1.97±0.
             10(stat)±0.21(syst), which is consistent with previous
             measurements. © 2006 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.96.191801},
   Key = {fds361223}
}

@article{fds321127,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Measurement of the relative width difference of the
             B0‐ B¯ 0 system with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2016)081},
   Abstract = {Abstract: This paper presents the measurement of the
             relative width difference ΔΓd/Γd of the B0‐ B¯ 0
             system using the data collected by the ATLAS experiment at
             the LHC in pp collisions at s=7 TeV and s=8 TeV and
             corresponding to an integrated luminosity of 25.2 fb−1.
             The value of ΔΓd/Γd is obtained by comparing the
             decay-time distributions of B0 → J/ψKS and B0 →
             J/ψK*0(892) decays. The result is ΔΓd/Γd = (−0.1±1.1
             (stat.)± 0.9 (syst.)) × 10−2. Currently, this is the
             most precise single measurement of ΔΓd/Γd. It agrees with
             the Standard Model prediction and the measurements by other
             experiments.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP06(2016)081},
   Key = {fds321127}
}

@article{fds373906,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
             J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
             Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
             GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
             M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
             JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
             C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
             KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena,
             E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster,
             AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio,
             S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos,
             G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
             K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
             L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry,
             T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov,
             VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans,
             G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
             EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
             AR and Cabras, G and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura,
             P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet,
             D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
             JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
             Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
             J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
             A},
   Title = {Measurement of the Sensitivity of Two-Particle Correlations
             in pp Collisions to the Presence of Hard
             Scatterings.},
   Journal = {Physical review letters},
   Volume = {131},
   Number = {16},
   Pages = {162301},
   Year = {2023},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.131.162301},
   Abstract = {A key open question in the study of multiparticle production
             in high-energy pp collisions is the relationship between the
             "ridge"-i.e., the observed azimuthal correlations between
             particles in the underlying event that extend over all
             rapidities-and hard or semihard scattering processes. In
             particular, it is not known whether jets or their soft
             fragments are correlated with particles in the underlying
             event. To address this question, two-particle correlations
             are measured in pp collisions at sqrt[s]=13  TeV using
             data collected by the ATLAS experiment at the LHC, with an
             integrated luminosity of 15.8  pb^{-1}, in two different
             configurations. In the first case, charged particles
             associated with jets are excluded from the correlation
             analysis, while in the second case, correlations are
             measured between particles within jets and charged particles
             from the underlying event. Second-order flow coefficients,
             v_{2}, are presented as a function of event multiplicity and
             transverse momentum. These measurements show that excluding
             particles associated with jets does not affect the measured
             correlations. Moreover, particles associated with jets do
             not exhibit any significant azimuthal correlations with the
             underlying event, ruling out hard processes contributing to
             the ridge.},
   Doi = {10.1103/physrevlett.131.162301},
   Key = {fds373906}
}

@booklet{Abbott98h,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
             EW and Astur, R and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
             K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
             SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
             Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {Measurement of the shape of the transverse momentum
             distribution of W bosons produced in pp¯ collisions at √s
             = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {25},
   Pages = {5498-5503},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.5498},
   Abstract = {The shape of the transverse momentum distribution of W
             bosons (pWT) produced in pp¯ collisions at √s = 1.8 TeV
             is measured with the D0 detector at Fermilab. The result is
             compared with QCD perturbative and resummation calculations
             over the pWT range from 0 to 200 GeV/c. The shape of the
             distribution is consistent with the theoretical prediction.
             © 1998 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.80.5498},
   Key = {Abbott98h}
}

@article{fds347514,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Measurement of the single top quark production cross section
             and},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {3},
   Year = {2016},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.032011},
   Abstract = {An updated measurement of the single top quark production
             cross section is presented using the full data set collected
             by the Collider Detector at Fermilab (CDF), corresponding to
             9.5 fb-1 of integrated luminosity from proton-antiproton
             collisions at 1.96 TeV center-of-mass energy. The events
             selected contain an imbalance in the total transverse
             momentum, jets identified as containing b quarks, and no
             identified leptons. The sum of the s- and t-channel single
             top quark cross sections is measured to be 3.53-1.16+1.25 pb
             and a lower limit on the magnitude of the top-to-bottom
             quark coupling, |Vtb| of 0.63, is obtained at the 95%
             credibility level. These measurements are combined with
             previously reported CDF results obtained from events with an
             imbalance in total transverse momentum, jets identified as
             originating from b quarks, and one identified lepton. The
             combined cross section is measured to be 3.02-0.48+0.49 pb
             and a lower limit on |Vtb| of 0.84 is obtained at the 95%
             credibility level.},
   Doi = {10.1103/PhysRevD.93.032011},
   Key = {fds347514}
}

@article{fds313620,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo,
             N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Galloni, C and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn,
             SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hirschbuehl, D and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino,
             P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon,
             CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat,
             P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano,
             I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Measurement of the single top quark production cross section
             and |Vtb| in events with one charged lepton, large missing
             transverse energy, and jets at CDF.},
   Journal = {Physical review letters},
   Volume = {113},
   Number = {26},
   Pages = {261804},
   Year = {2014},
   Month = {December},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.113.261804},
   Abstract = {We report a measurement of single top quark production in
             proton-antiproton collisions at a center-of-mass energy of
             sqrt[s]=1.96  TeV using a data set corresponding to
             7.5  fb(-1) of integrated luminosity collected by the
             Collider Detector at Fermilab. We select events consistent
             with the single top quark decay process t→Wb→ℓνb by
             requiring the presence of an electron or muon, a large
             imbalance of transverse momentum indicating the presence of
             a neutrino, and two or three jets including at least one
             originating from a bottom quark. An artificial neural
             network is used to discriminate the signal from backgrounds.
             We measure a single top quark production cross section of
             3.04(-0.53)(+0.57)  pb and set a lower limit on the
             magnitude of the coupling between the top quark and bottom
             quark |Vtb|>0.78 at the 95% credibility level.},
   Doi = {10.1103/physrevlett.113.261804},
   Key = {fds313620}
}

@article{fds308003,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the Single-Top-Quark Production Cross Section
             at CDF},
   Journal = {Physical Review Letters},
   Volume = {101},
   Number = {25},
   Pages = {252001},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.252001},
   Abstract = {We report a measurement of the single-top-quark production
             cross section in 2.2  fb-1 of pp̅ collision data
             collected by the Collider Detector at Fermilab at
             sqrt[s]=1.96  TeV. Candidate events are classified as
             signal-like by three parallel analyses which use likelihood,
             matrix element, and neural network discriminants. These
             results are combined in order to improve the sensitivity. We
             observe a signal consistent with the standard model
             prediction, but inconsistent with the background-only model
             by 3.7 standard deviations with a median expected
             sensitivity of 4.9 standard deviations. We measure a cross
             section of 2.2-0.6+0.7(stat+syst)  pb, extract the
             Cabibbo-Kobayashi-Maskawa matrix-element value
             |Vtb|=0.88-0.12+0.13(stat+syst) &plusmn; 0.07(theory), and
             set the limit |Vtb|&gt;0.66 at the 95% C.L.},
   Doi = {10.1103/physrevlett.101.252001},
   Key = {fds308003}
}

@article{fds347459,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
             P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
             H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
             C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
             AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
             O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
             R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
             JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran,
             J},
   Title = {Measurement of the Soft-Drop Jet Mass in pp Collisions at
             sqrt[s]=13  TeV with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {121},
   Number = {9},
   Pages = {092001},
   Year = {2018},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.121.092001},
   Abstract = {Jet substructure observables have significantly extended the
             search program for physics beyond the standard model at the
             Large Hadron Collider. The state-of-the-art tools have been
             motivated by theoretical calculations, but there has never
             been a direct comparison between data and calculations of
             jet substructure observables that are accurate beyond
             leading-logarithm approximation. Such observables are
             significant not only for probing the collinear regime of QCD
             that is largely unexplored at a hadron collider, but also
             for improving the understanding of jet substructure
             properties that are used in many studies at the Large Hadron
             Collider. This Letter documents a measurement of the first
             jet substructure quantity at a hadron collider to be
             calculated at next-to-next-to-leading-logarithm accuracy.
             The normalized, differential cross section is measured as a
             function of log_{10}ρ^{2}, where ρ is the ratio of the
             soft-drop mass to the ungroomed jet transverse momentum.
             This quantity is measured in dijet events from
             32.9  fb^{-1} of sqrt[s]=13  TeV proton-proton
             collisions recorded by the ATLAS detector. The data are
             unfolded to correct for detector effects and compared to
             precise QCD calculations and leading-logarithm
             particle-level Monte Carlo simulations.},
   Doi = {10.1103/physrevlett.121.092001},
   Key = {fds347459}
}

@article{fds356651,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A},
   Title = {Measurement of the suppression and azimuthal anisotropy of
             muons from heavy-flavor decays in Pb+Pb collisions at sNN
             =2.76 TeV with the ATLAS detector},
   Journal = {Physical Review C},
   Volume = {98},
   Number = {4},
   Year = {2018},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevC.98.044905},
   Abstract = {ATLAS measurements of the production of muons from
             heavy-flavor decays in sNN=2.76 TeV Pb+Pb collisions and
             s=2.76 TeV pp collisions at the LHC are presented.
             Integrated luminosities of 0.14 nb-1 and 570 nb-1 are used
             for the Pb+Pb and pp measurements, respectively, which are
             performed over the muon transverse momentum range 4<pT<14
             GeV and for five Pb+Pb centrality intervals. Backgrounds
             arising from in-flight pion and kaon decays, hadronic
             showers, and misreconstructed muons are statistically
             removed using a template-fitting procedure. The heavy-flavor
             muon differential cross sections and per-event yields are
             measured in pp and Pb+Pb collisions, respectively. The
             nuclear modification factor RAA obtained from these is
             observed to be independent of pT, within uncertainties, and
             to be less than unity, which indicates suppressed production
             of heavy-flavor muons in Pb+Pb collisions. For the 10% most
             central Pb+Pb events, the measured RAA is approximately
             0.35. The azimuthal modulation of the heavy-flavor muon
             yields is also measured and the associated Fourier
             coefficients vn for n=2, 3, and 4 are given as a function of
             pT and centrality. They vary slowly with pT and show a
             systematic variation with centrality which is characteristic
             of other anisotropy measurements, such as that observed for
             inclusive hadrons. The measured RAA and vn values are also
             compared with theoretical calculations.},
   Doi = {10.1103/PhysRevC.98.044905},
   Key = {fds356651}
}

@article{fds308128,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the t anti-t production cross section in
             $p\bar{p}$ collisions at $\sqrt{s} =$ 1.96-TeV in the all
             hadronic decay mode},
   Journal = {Phys. Rev.},
   Volume = {D74},
   Number = {7},
   Pages = {072005},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.74.072005},
   Abstract = {We report a measurement of the tt-bar production cross
             section using the CDF II detector at the Fermilab Tevatron.
             The analysis is performed using 322 pb-1 of p anti-p
             collisions at s**(1/2) = 1.96 TeV. The data consist of
             events selected with six or more hadronic jets with
             additional kinematic requirements. At least one of these
             jets must be identified as a b-quark jet by the
             reconstruction of a secondary vertex. The cross section is
             measured to be sigma_tt-bar = 7.5 +/- 2.1(stat.)+3.3_-2.2(syst.)+0.5_-0.4(lumi.)
             pb, which is consistent with the standard model
             prediction.},
   Doi = {10.1103/PhysRevD.74.072005},
   Key = {fds308128}
}

@article{fds308120,
   Author = {Acosta, and D, and others},
   Title = {Measurement of the t anti-t production cross section in p
             anti-p collisions at sqrt[s]=1.96 TeV using lepton + jets
             events with secondary vertex b-tagging},
   Journal = {Phys. Rev.},
   Volume = {D71},
   Number = {7},
   Pages = {052003},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.74.072006},
   Abstract = {http://arxiv.org/abs/hep-ex/0410041},
   Doi = {10.1103/PhysRevD.74.072006},
   Key = {fds308120}
}

@article{fds356755,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu,
             H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik,
             M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O},
   Title = {Measurement of the t t production cross section in the
             τ+jets final state in pp collisions at s =8 TeV using the
             ATLAS detector},
   Journal = {Physical Review D},
   Volume = {95},
   Number = {7},
   Year = {2017},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.95.072003},
   Abstract = {A measurement of the inclusive pp→tt+X production cross
             section in the τ+jets final state using only the hadronic
             decays of the τ lepton is presented. The measurement is
             performed using 20.2 fb-1 of proton-proton collision data
             recorded at a center-of-mass energy of s=8 TeV with the
             ATLAS detector at the Large Hadron Collider. The cross
             section is measured via a counting experiment by imposing a
             set of selection criteria on the identification and
             kinematic variables of the reconstructed particles and jets,
             and on event kinematic variables and characteristics. The
             production cross section is measured to be σtt=239±29 pb,
             which is in agreement with the measurements in other final
             states and the theoretical predictions at this
             center-of-mass energy.},
   Doi = {10.1103/PhysRevD.95.072003},
   Key = {fds356755}
}

@article{fds359997,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S and Arling, JH},
   Title = {Measurement of the t t¯ t t¯ production cross section in
             pp collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {11},
   Year = {2021},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2021)118},
   Abstract = {A measurement of four-top-quark production using
             proton-proton collision data at a centre-of-mass energy of
             13 TeV collected by the ATLAS detector at the Large Hadron
             Collider corresponding to an integrated luminosity of 139
             fb−1 is presented. Events are selected if they contain a
             single lepton (electron or muon) or an opposite-sign lepton
             pair, in association with multiple jets. The events are
             categorised according to the number of jets and how likely
             these are to contain b-hadrons. A multivariate technique is
             then used to discriminate between signal and background
             events. The measured four-top-quark production cross section
             is found to be 26−15+17 fb, with a corresponding observed
             (expected) significance of 1.9 (1.0) standard deviations
             over the background-only hypothesis. The result is combined
             with the previous measurement performed by the ATLAS
             Collaboration in the multilepton final state. The combined
             four-top-quark production cross section is measured to be
             24−6+7 fb, with a corresponding observed (expected) signal
             significance of 4.7 (2.6) standard deviations over the
             background-only predictions. It is consistent within 2.0
             standard deviations with the Standard Model expectation of
             12.0 ± 2.4 fb. [Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP11(2021)118},
   Key = {fds359997}
}

@article{fds307777,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Measurement of the t-channel single top-quark production
             cross section in pp collisions at s=7 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {717},
   Number = {4-5},
   Pages = {330-350},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.09.031},
   Abstract = {We report a measurement of the cross section of single
             top-quark production in the t-channel using 1.04 fb−1 of
             pp collision data at s=7 TeV recorded with the ATLAS
             detector at the LHC. Selected events feature one electron or
             muon, missing transverse momentum, and two or three jets,
             exactly one of them identified as originating from a b
             quark. The cross section is measured by fitting the
             distribution of a multivariate discriminant constructed with
             a neural network, yielding σt=83±4(stat.)−19+20(syst.)
             pb, which is in good agreement with the prediction of the
             Standard Model. Using the ratio of the measured to the
             theoretically predicted cross section and assuming that the
             top-quark-related CKM matrix elements obey the relation
             |Vtb|≫|Vts|,|Vtd|, the coupling strength at the W-t-b
             vertex is determined to be |Vtb|=1.13−0.13+0.14. If it is
             assumed that |Vtb|⩽1 a lower limit of |Vtb|>0.75 is
             obtained at the 95% confidence level.},
   Doi = {10.1016/j.physletb.2012.09.031},
   Key = {fds307777}
}

@article{fds310279,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Measurement of the top pair production cross section in 8
             TeV proton-proton collisions using kinematic information in
             the lepton + jets final state with ATLAS},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.112013},
   Abstract = {A measurement is presented of the (formula presented)
             inclusive production cross section in pp collisions at a
             center-of-mass energy of (formula presented) using data
             collected by the ATLAS detector at the CERN Large Hadron
             pffiffi Collider. The measurement was performed in the
             lepton + jets final state using a data set corresponding to
             an integrated luminosity of 20.3 fb-1. The cross section was
             obtained using a likelihood discriminant fit and b-jet
             identification was used to improve the signal-to-background
             ratio. The inclusive tt production cross section was
             measured to be (formula presented) pb assuming a top-quark
             mass of 172.5 GeV, in good agreement with the theoretical
             prediction of (formula presented) pb. The (formula
             presented) production cross section in the fiducial region
             determined by the detector acceptance is also
             reported.},
   Doi = {10.1103/PhysRevD.91.112013},
   Key = {fds310279}
}

@article{fds307881,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of the top pair production cross section in the
             $\mathrm{{lepton}}+\mathrm{{jets}}$ channel using a jet
             flavor discriminant},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {3},
   Pages = {031101},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.031101},
   Abstract = {We present a new method to measure the top quark pair
             production cross section and the background rates with data
             corresponding to an integrated luminosity of 2.7fb-1 from
             pp̄ collisions at √s=1.96TeV collected with the CDF II
             Detector. We select events with a single electron or muon
             candidate, missing transverse energy, and at least one
             b-tagged jet. We perform a simultaneous fit to a jet flavor
             discriminant across nine samples defined by the number of
             jets and b tags. An advantage of this approach is that many
             systematic uncertainties are measured in situ and inversely
             scale with integrated luminosity. We measure a top cross
             section of σ tt̄=7.64±0.57(stat+syst)±0.45(luminosity)pb.
             © 2011 American Physical Society.},
   Doi = {10.1103/PhysRevD.84.031101},
   Key = {fds307881}
}

@article{fds307931,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the top pair production cross section in the
             dilepton decay channel in $pp[over \ifmmode\bar\else\textasciimacron\fi{}]$
             collisions at $\sqrt{s}=1.96\,\,TeV$},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {5},
   Pages = {052002},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.052002},
   Abstract = {A measurement of the tt̄ production cross section in pp̄
             collisions at √s=1.96TeV using events with two leptons,
             missing transverse energy, and jets is reported. The data
             were collected with the CDF II detector. The result in a
             data sample corresponding to an integrated luminosity
             2.8fb-1 is σtt̄=6.27±0.73(stat) ±0.63(syst)±0.39(lum)pb.
             for an assumed top mass of 175GeV/c2. © 2010 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.82.052002},
   Key = {fds307931}
}

@article{fds307565,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson,
             TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand,
             S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
   Title = {Measurement of the top quark charge in pp collisions at √s
             = 7 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP11(2013)031},
   Abstract = {A measurement of the top quark electric charge is carried
             out in the ATLAS experiment at the Large Hadron Collider
             using 2.05 fb-1 of data at a centre-of-mass energy of 7TeV.
             In units of the elementary electric charge, the top quark
             charge is determined to be 0.64 ± 0.02 (stat.) ± 0.08
             (syst.) from the charges of the top quark decay products in
             single lepton tt̄ candidate events. This excludes models
             that propose a heavy quark of electric charge -4/3, instead
             of the Standard Model top quark, with a significance of more
             than 8σ. Copyright CERN.},
   Doi = {10.1007/JHEP11(2013)031},
   Key = {fds307565}
}

@article{fds307603,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Measurement of the top quark forward-backward production
             asymmetry and its dependence on event kinematic
             properties},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {9},
   Pages = {092002},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.092002},
   Abstract = {We present new measurements of the inclusive
             forward-backward tt̄ production asymmetry, AFB, and its
             dependence on several properties of the tt̄ system. The
             measurements are performed with the full Tevatron data set
             recorded with the CDF II detector during pp̄ collisions at
             √s=1.96 TeV, corresponding to an integrated luminosity of
             9.4 fb -1. We measure the asymmetry using the rapidity
             difference Δy=yt-yt̄. Parton-level results are derived,
             yielding an inclusive asymmetry of 0.164±0.047(stat+syst).
             We establish an approximately linear dependence of AFB on
             the top-quark pair mass Mtt̄ and the rapidity difference
             |Δy| at detector and parton levels. Assuming the standard
             model, the probabilities to observe the measured values or
             larger for the detector-level dependencies are 7.4×10-3 and
             2.2×10-3 for Mtt̄ and |Δy| respectively. Lastly, we study
             the dependence of the asymmetry on the transverse momentum
             of the tt̄ system at the detector level. These results are
             consistent with previous lower-precision measurements and
             provide additional quantification of the functional
             dependencies of the asymmetry. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.87.092002},
   Key = {fds307603}
}

@article{fds307922,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the Top Quark Mass and $p \bar{p} \to t
             \bar{t}$ Cross Section in the All-Hadronic Mode with the
             CDFII Detector},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {5},
   Pages = {052011},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.052011},
   Abstract = {http://arxiv.org/abs/1002.0365},
   Doi = {10.1103/PhysRevD.81.052011},
   Key = {fds307922}
}

@article{fds307984,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the top quark mass at CDF using the
             ``neutrino phi weighting'' template method on a lepton plus
             isolated track sample},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {7},
   Pages = {072005},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.072005},
   Abstract = {We present a measurement of the top quark mass with tt̄
             dilepton events produced in pp̄ collisions at the Fermilab
             Tevatron (s=1.96TeV) and collected by the CDF II detector. A
             sample of 328 events with a charged electron or muon and an
             isolated track, corresponding to an integrated luminosity of
             2.9fb-1, are selected as tt̄ candidates. To account for the
             unconstrained event kinematics, we scan over the phase space
             of the azimuthal angles (ν1,ν2) of neutrinos and
             reconstruct the top quark mass for each ν1, ν2 pair by
             minimizing a χ2 function in the tt̄ dilepton hypothesis.
             We assign χ2-dependent weights to the solutions in order to
             build a preferred mass for each event. Preferred mass
             distributions (templates) are built from simulated tt̄ and
             background events, and parametrized in order to provide
             continuous probability density functions. A likelihood fit
             to the mass distribution in data as a weighted sum of signal
             and background probability density functions gives a top
             quark mass of 165.5-3.3+3.4(stat)±3. 1(syst)GeV/c2. © 2009
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.79.072005},
   Key = {fds307984}
}

@article{fds308070,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the Top Quark Mass in $p\bar{p}$Collisions at
             $\sqrt{s} = 1.96$ TeV using the Decay Length
             Technique},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {7},
   Pages = {071102},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.071102},
   Abstract = {We report the first measurement of the top quark mass using
             the decay length technique in p[overline p] collisions at a
             center-of-mass energy of 1.96 TeV. This technique uses the
             measured flight distance of the b hadron to infer the mass
             of the top quark in lepton plus jets events with missing
             transverse energy. It relies solely on tracking and avoids
             the jet energy scale uncertainty that is common to all other
             methods used so far. We apply our novel method to a 695 pb-1
             data sample recorded by the CDF II detector at Fermilab and
             extract a measurement of mt=180.7-13.4+15.5(stat.)$\pm$8.6(syst.)
             GeV/c2. While the uncertainty of this result is larger than
             that of other measurements, the dominant uncertainties in
             the decay length technique are uncorrelated with those in
             other methods. This result can help reduce the overall
             uncertainty when combined with other existing measurements
             of the top quark mass.},
   Doi = {10.1103/PhysRevD.75.071102},
   Key = {fds308070}
}

@article{fds307822,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M},
   Title = {Measurement of the top quark mass in the all-hadronic mode
             at CDF},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {714},
   Number = {1},
   Pages = {24-31},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {July},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.06.007},
   Abstract = {A measurement of the top quark mass (M top) in the
             all-hadronic decay channel is presented. It uses 5.8 fb -1
             of pp data collected with the CDF II detector at the
             Fermilab Tevatron Collider. Events with six to eight jets
             are selected by a neural network algorithm and by the
             requirement that at least one of the jets is tagged as a
             b-quark jet. The measurement is performed with a likelihood
             fit technique, which simultaneously determines M top and the
             jet energy scale (JES) calibration. The fit yields a value
             of M top=172.5±1.4(stat)±1.0(JES)±1.1(syst) GeV/c 2. ©
             2012 Elsevier B.V.},
   Doi = {10.1016/j.physletb.2012.06.007},
   Key = {fds307822}
}

@article{fds308213,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Balamurali, V and Baldin, B and Banerjee,
             S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding,
             F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey,
             D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang,
             SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger,
             C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
             P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
             G},
   Title = {Measurement of the top quark mass in the dilepton
             channel},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {60},
   Number = {5},
   Pages = {1-21},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.60.052001},
   Abstract = {We report a measurement of the top quark mass using six
             candidate events for the process (Formula presented),
             observed in the D0 experiment at the Fermilab (Formula
             presented) collider. Using maximum likelihood fits to the
             dynamics of the decays, we measure a mass for the top quark
             of (Formula presented). We combine this result with our
             previous measurement in the (Formula presented) channel to
             obtain (Formula presented) as the best value of the mass of
             the top quark measured by D0. © 1999 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.60.052001},
   Key = {fds308213}
}

@article{fds307885,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R},
   Title = {Measurement of the top quark mass in the lepton+jets channel
             using the lepton transverse momentum},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {698},
   Number = {5},
   Pages = {371-379},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.03.041},
   Abstract = {This Letter reports a measurement of the top quark mass,
             Mtop, in data from pp- collisions at s=1.96 TeV
             corresponding to 2.7 fb-1 of integrated luminosity at the
             Fermilab Tevatron using the CDF II detector. Events with the
             lepton+jets topology are selected. An unbinned likelihood is
             constructed based on the dependence of the lepton transverse
             momentum, PT, on Mtop. A maximum likelihood fit to the data
             yields a measured mass Mtop=176.9±8.0stat±2.7syst GeV/c2.
             In this measurement, the contribution by the jet energy
             scale uncertainty to the systematic error is negligible. The
             result provides an important consistency test for other Mtop
             measurements where explicit use of the jet energy is made
             for deriving the top quark mass. © 2011 Elsevier
             B.V.},
   Doi = {10.1016/j.physletb.2011.03.041},
   Key = {fds307885}
}

@article{fds356610,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella, L and Arabidze, G and Araque,
             JP and Araujo Ferraz, V and Araujo Pereira, R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ},
   Title = {Measurement of the top quark mass in the tt¯ →
             lepton+jets channel from √s=8 TeV ATLAS data and
             combination with previous results},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {4},
   Year = {2019},
   Month = {April},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-6757-9},
   Abstract = {The top quark mass is measured using a template method in
             the tt¯ → lepton + jets channel (lepton is e or μ) using
             ATLAS data recorded in 2012 at the LHC. The data were taken
             at a proton–proton centre-of-mass energy of s=8 TeV and
             correspond to an integrated luminosity of 20.2 fb - 1 . The
             tt¯ → lepton + jets channel is characterized by the
             presence of a charged lepton, a neutrino and four jets, two
             of which originate from bottom quarks (b). Exploiting a
             three-dimensional template technique, the top quark mass is
             determined together with a global jet energy scale factor
             and a relative b-to-light-jet energy scale factor. The mass
             of the top quark is measured to be mtop=172.08±0.39(stat)±0.82(syst) GeV.
             A combination with previous ATLAS m top measurements gives
             mtop=172.69±0.25(stat)±0.41(syst) GeV.},
   Doi = {10.1140/epjc/s10052-019-6757-9},
   Key = {fds356610}
}

@article{fds321133,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of the top quark mass in the tt¯→dilepton
             channel from √s=8 TeV ATLAS data},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {761},
   Pages = {350-371},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.08.042},
   Abstract = {The top quark mass is measured in the tt¯→dilepton
             channel (lepton=e,μ) using ATLAS data recorded in the year
             2012 at the LHC. The data were taken at a proton–proton
             centre-of-mass energy of s=8 TeV and correspond to an
             integrated luminosity of about 20.2 fb−1. Exploiting the
             template method, and using the distribution of invariant
             masses of lepton–b-jet pairs, the top quark mass is
             measured to be mtop=172.99±0.41 (stat)±0.74 (syst) GeV,
             with a total uncertainty of 0.84 GeV. Finally, a combination
             with previous ATLAS mtop measurements from s=7 TeV data in
             the tt¯→dilepton and tt¯→lepton+jets channels results
             in mtop=172.84±0.34 (stat)±0.61 (syst) GeV, with a total
             uncertainty of 0.70 GeV.},
   Doi = {10.1016/j.physletb.2016.08.042},
   Key = {fds321133}
}

@article{fds310333,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
             G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA},
   Title = {Measurement of the top quark mass in the [Formula: see text]
             and [Formula: see text] channels using [Formula: see
             text] [Formula: see text] ATLAS data.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {330},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3544-0},
   Doi = {10.1140/epjc/s10052-015-3544-0},
   Key = {fds310333}
}

@booklet{Abbott98m,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
             V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
             HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros, Y and Dudko,
             LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga, MK and Featherly,
             J and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk,
             HE},
   Title = {Measurement of the top quark mass using dilepton
             events},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {10},
   Pages = {2063-2068},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.2063},
   Abstract = {The D0 Collaboration has performed a measurement of the top
             quark mass mt based on six candidate events for the process
             tt- → bW+bW-, where the W bosons decay to eν or μν.
             This sample was collected during an exposure of the D0
             detector to an integrated luminosity of 125pb-1 of √ s =
             1.8 TeV pp collisions. We obtain mt = 168.4 ± 12.3(stat) ±
             3.6(syst) GeV/c2, consistent with the measurement obtained
             using single-lepton events. Combination of the single-lepton
             and dilepton results yields mt = 172.0 ± 7.5 GeV/c2. ©
             1998 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.80.2063},
   Key = {Abbott98m}
}

@article{fds308124,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the top quark mass using template methods on
             dilepton events in proton antiproton collisions at $\sqrt{s}
             =$ 1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D73},
   Number = {11},
   Pages = {112006},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.112006},
   Abstract = {We describe a measurement of the top quark mass from events
             produced in p anti-p collisions at a center-of-mass energy
             of 1.96 TeV, using the Collider Detector at Fermilab. We
             identify tt-bar candidates where both W bosons from the top
             quarks decay into leptons (e mu, mu nu, or tau nu) from a
             data sample of 360 pb-1. The top quark mass is reconstructed
             in each event separately by three different methods, which
             draw upon simulated distributions of the neutrino
             pseudorapi+dity, tt-bar longitudinal momentum, or neutrino
             azimuthal angle in order to extract probability
             distributions for the top quark mass. For each method,
             representative mass distributions, or templates, are
             constructed from simulated samples of signal and background
             events, and parametrized templates is then performed on the
             data sample masses in order to derive a final top quark
             mass. Combining the three template methods, taking into
             account correlations in their statistical and systematic
             uncertainties, results in a top quark mass measurement of
             170.1 +/- 6.0 (stat.) +/- 4.1 (syst.) GeV/c2.},
   Doi = {10.1103/PhysRevD.73.112006},
   Key = {fds308124}
}

@article{fds307985,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the top quark mass using the invariant mass
             of lepton pairs in soft muon b-tagged events},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {5},
   Pages = {051104},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.051104},
   Abstract = {We present the first measurement of the mass of the top
             quark in a sample of tt̅ →ℓν̅ bb̅ qq̅ events (where
             ℓ=e,μ) selected by identifying jets containing a muon
             candidate from the semileptonic decay of heavy-flavor
             hadrons (soft muon b tagging). The pp̅ collision data used
             correspond to an integrated luminosity of 2  fb-1 and
             were collected by the CDF II detector at the Fermilab
             Tevatron Collider. The measurement is based on a novel
             technique exploiting the invariant mass of a subset of the
             decay particles, specifically the lepton from the W boson of
             the t→Wb decay and the muon from a semileptonic b decay.
             We fit template histograms, derived from simulation of tt̅
             events and a modeling of the background, to the mass
             distribution observed in the data and measure a top quark
             mass of 180.5 &plusmn; 12.0(stat) &plusmn;
             3.6(syst)  GeV/c2, consistent with the current world
             average value.},
   Doi = {10.1103/PhysRevD.80.051104},
   Key = {fds307985}
}

@article{fds307959,
   Author = {al, AVKWTAE and Collaboration, CDF},
   Title = {Measurement of the top quark mass with dilepton events
             selected using neuroevolution at CDF},
   Journal = {Physical Review Letters},
   Volume = {102},
   Number = {152001},
   Pages = {6},
   Year = {2009},
   Month = {Spring},
   Key = {fds307959}
}

@article{fds308113,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the top quark mass with the dynamical
             likelihood method using lepton plus jets events with b-tags
             in $p\bar{p}$ collisions at $\sqrt{s} =$
             1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D73},
   Number = {9},
   Pages = {092002},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.092002},
   Abstract = {This report describes a measurement of the top quark mass,
             M_top, with the dynamical likelihood method (DLM) using the
             CDF II detector at the Fermilab Tevatron. The Tevatron
             produces top/anti-top (t anti-t) pairs in p anti-p
             collisions at a center-of-mass energy of 1.96 TeV. The data
             sample used in this analysis was accumulated from March 2002
             through August 2004, which corresponds to an integrated
             luminosity of 318 pb-1. We use the tt-bar candidates in the
             ``epton+jets'' decay channel, requiring at least one jet
             identified as a b quark by finding a displaced secondary
             vertex. The DLM defines a likelihood for each event based on
             the differential cross section s a function of M_top per
             unit phase space volume of the final partons, multiplied by
             the transfer functions from jet to parton energies. The
             method takes into account all possible jet combinations in
             an event, and the likelihood is multiplied event by event to
             derive the top quark mass by the maximum likelihood method.
             Using 63 tt-bar candidates observed in the data, with 9.2
             events expected from background, we measure the top quark
             mass to be 173.2+2.6_-2.4 (stat.) +/- 3.2 (syst.) GeV/c2, or
             173+4.1_-4.0 GeV/c2.},
   Doi = {10.1103/PhysRevD.73.092002},
   Key = {fds308113}
}

@article{fds307722,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard,
             R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli,
             F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji,
             W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi,
             M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC},
   Title = {Measurement of the top quark mass with the template method
             in the [Formula: see text] channel using ATLAS
             data.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {72},
   Number = {6},
   Pages = {2046},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2046-6},
   Abstract = {The top quark mass has been measured using the template
             method in the [Formula: see text] channel based on data
             recorded in 2011 with the ATLAS detector at the LHC. The
             data were taken at a proton-proton centre-of-mass energy of
             [Formula: see text] and correspond to an integrated
             luminosity of 1.04 fb<sup>-1</sup>. The analyses in the
             <i>e</i>+jets and <i>μ</i>+jets decay channels yield
             consistent results. The top quark mass is measured to be
             <i>m</i><sub>top</sub>=174.5±0.6<sub>stat</sub>±2.3<sub>syst</sub>
             GeV.},
   Doi = {10.1140/epjc/s10052-012-2046-6},
   Key = {fds307722}
}

@article{fds307790,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós,
             G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi,
             F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
             A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
             S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans,
             G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
             M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
             T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins, NJ and Collins-Tooth, C and Collot,
             J and Colombo, T},
   Title = {Measurement of the top quark pair cross section with ATLAS
             in pp collisions at s=7 TeV using final states with an
             electron or a muon and a hadronically decaying τ
             lepton},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {717},
   Number = {1-3},
   Pages = {89-108},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.09.032},
   Abstract = {A measurement of the cross section of top quark pair
             production in proton-proton collisions recorded with the
             ATLAS detector at the Large Hadron Collider at a
             centre-of-mass energy of 7 TeV is reported. The data sample
             used corresponds to an integrated luminosity of 2.05 fb-1.
             Events with an isolated electron or muon and a τ lepton
             decaying hadronically are used. In addition, a large missing
             transverse momentum and two or more energetic jets are
             required. At least one of the jets must be identified as
             originating from a b quark. The measured cross section,
             σtt-=186±13(stat.)±20(syst.)±7(lumi.) pb, is in good
             agreement with the Standard Model prediction. © 2012
             CERN.},
   Doi = {10.1016/j.physletb.2012.09.032},
   Key = {fds307790}
}

@article{fds307551,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
             S},
   Title = {Measurement of the top quark pair production charge
             asymmetry in proton-proton collisions at √s = 7 TeV using
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {2},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP02(2014)107},
   Abstract = {This paper presents a measurement of the top quark pair
             (tt̄) production charge asymmetry AC using 4.7 fb-1 of
             proton-proton collisions at a centre-of-mass energy √s =
             7TeV collected by the ATLAS detector at the LHC. A
             tt̄-enriched sample of events with a single lepton
             (electron or muon), missing transverse momentum and at least
             four high transverse momentum jets, of which at least one is
             tagged as coming from a b-quark, is selected. A likelihood
             fit is used to reconstruct the tt̄ event kinematics. A
             Bayesian unfolding procedure is employed to estimate AC at
             the parton-level. The measured value of the tt̄ production
             charge asymmetry is AC = 0.006 ± 0.010, where the
             uncertainty includes both the statistical and the systematic
             components. Differential AC measurements as a function of
             the invariant mass, the rapidity and the transverse momentum
             of the tt̄- system are also presented. In addition, AC is
             measured for a subset of events with large tt̄ velocity,
             where physics beyond the Standard Model could contribute.
             All measurements are consistent with the Standard Model
             predictions.},
   Doi = {10.1007/JHEP02(2014)107},
   Key = {fds307551}
}

@article{fds307749,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the top quark pair production cross section
             in pp collisions at √s=7TeV in dilepton final states with
             ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {707},
   Number = {5},
   Pages = {459-477},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.12.055},
   Abstract = {A measurement of the production cross section of top quark
             pairs (tt̄) in proton-proton collisions at a center-of-mass
             energy of 7 TeV recorded with the ATLAS detector at the
             Large Hadron Collider is reported. Candidate events are
             selected in the dilepton topology with large missing
             transverse energy and at least two jets. Using a data sample
             corresponding to an integrated luminosity of 35pb-1, a tt̄
             production cross section σtt̄=177±20(stat.)±14(syst.)±7(lum.)pb
             is measured for an assumed top quark mass of mt=172.5GeV. A
             second measurement requiring at least one jet identified as
             coming from a b quark yields a comparable result,
             demonstrating that the dilepton final states are consistent
             with being accompanied by b-quark jets. These measurements
             are in good agreement with Standard Model predictions. ©
             2011 CERN.},
   Doi = {10.1016/j.physletb.2011.12.055},
   Key = {fds307749}
}

@article{fds308215,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon,
             R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Signore, KD and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Loreto, GD and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland,
             T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Gavrilov, V and Geld, TL and II, RJG and Genser, K and Gerber, CE and Gershtein, Y and Gibbard, B and Gobbi, B and Gómez, B and Gómez, G and Goncharov, PI and Solís, JLG and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Grannis, PD and Green, DR and Greenlee, H and Grinstein, S and Grudberg, P and Grünendahl, S and Guglielmo, G and Guida, JA and Guida, JM and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hedin, D and Heinson, AP and Heintz, U and Hernández-Monloya, R and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hsieh, F and Hu, T and Ito, AS and Jaques,
             J and Jerger, SA and Jesik, R and Joffe-Minor, T and Johns, K and Johnson,
             M and Jonckheere, A and Jones, M and Jöstlein, H and Jun, SY and Jung, CK and Kahn, S and Kalbfleisch, G and Karmanov, D and Karmgard, D and Kehoe, R and Kelly, ML and Kim, SK and Klima, B and Klopfenstein, C and Ko, W and Kohli,
             JM and Koltick, D and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kuleshov, S and Kulik, Y and Kunori, S and Landry,
             F and Landsberg, G and Lauer, B and Leflat, A and Li, J and Li, QZ and Lima,
             JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lobkowicz, F and Loken, SC and Lucotte, A and Lueking, L and Lyon, AL and Maciel, AKA and Madaras, RJ and Madden, R and Magaña-Mendoza, L and Manankov, V and Mani, S and Mao, HS and Markeloff, R and Marshall, T and Martin, MI and Mauritz, KM and May, B and Mayorov, AA and McCarthy, R and McDonald, J and McKibben, T and McKinley, J and McMahon, T and Melanson,
             HL and Merkin, M and Merritt, KW and Miao, C and Miettinen, H and Mincer,
             A and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery, HE and Mooney, P and Moromisato, J and Mostafa, M and Motta, HD and Murphy, C and Nang, F and Narain, M and Narasimham, VS and Narayanan, A and Neal, HA and Negret, JP and Nemethy, P and Norman, D and Oesch, L and Oguri, V and Oliveira, E and Oltman, E and Oshima, N and Owen, D and Padley, P and Para,
             A and Park, YM and Partridge, R and Parua, N and Paterno, M and Pawlik, B and Perkins, J and Peters, M and Piegaia, R and Piekarz, H and Pischalnikov,
             Y and Pope, BG and Prosper, HB and Protopopescu, S and Qian, J and Quintas,
             PZ and Raja, R and Rajagopalan, S and Ramirez, O and Reucroft, S and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Sánchez-Hernández, A and Santoro, A and Sawyer,
             L and Schamberger, RD and Schellman, H and Sculli, J and Shabalina, E and Shaffer, C and Shankar, HC and Shivpuri, RK and Shpakov, D and Shupe, M and Singh, H and Singh, JB and Sirotenko, V and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sosebee, M and Sotnikova, N and Souza, M and Steinbrück, G and Stephens, RW and Stevenson, ML and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Streets, K and Strovink,
             M and Sznajder, A and Tamburello, P and Tarazi, J and Tartaglia, M and Thomas, TLT and Thompson, J and Trippe, TG and Tuts, PM and Vaniev, V and Varelas, N and Varnes, EW and Vititoe, D and Volkov, AA and Vorobiev,
             AP and Wahl, HD and Wang, G and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Wightman, JA and Willis, S and Wimpenny, SJ and Wirjawan, JVD and Womersley, J and Won, E and Wood, DR and Wu, Z and Yamada, R and Yamin, P and Yasuda, T and Yepes, P and Yip, K and Yoshikawa, C and Youssef, S and Yu, J and Yu, Y and Zhang, B and Zhou, Y and Zhou, Z and Zhu, ZH and Zielinski, M and Zieminska, D and Zieminski, A and Zverev, EG and Zylberstejn, A},
   Title = {Measurement of the top quark pair production cross section
             in pp̄ collisions using multijet final states},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {60},
   Number = {1},
   Pages = {1-26},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/PhysRevD.60.012001},
   Abstract = {We have studied tt̄ production using multijet final states
             in pp̄ collisions at a center-of-mass energy of 1.8 TeV,
             with an integrated luminosity of 110.3 pb-1. Each of the top
             quarks with these final states decays exclusively to a
             bottom quark and a W boson, with the W bosons decaying into
             quark-antiquark pairs. The analysis has been optimized using
             neural networks to achieve the smallest expected fractional
             uncertainty on the tt̄ production cross section, and yields
             a cross section of 7.1±2.8 (stat)±1.5 (syst) pb, assuming
             a top quark mass of 172.1 GeV/c2. Combining this result with
             previous DØ measurements, where one or both of the W bosons
             decay leptonically, gives a tt̄ production cross section of
             5.9±1.2 (stat)±1.1 (syst) pb. ©1999 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.60.012001},
   Key = {fds308215}
}

@booklet{Abachi97b,
   Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cumings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
             HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard, J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
             MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
             G},
   Title = {Measurement of the top quark pair production cross section
             in p¯p collisions},
   Journal = {Physical Review Letters},
   Volume = {79},
   Number = {7},
   Pages = {1203-1208},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.1203},
   Abstract = {We present a measurement of the t¯t production cross
             section in p¯p collisions at √s=1.8TeV by the D0
             experiment at the Fermilab Tevatron. The measurement is
             based on data from an integrated luminosity of approximately
             125pb−1 accumulated during the 1992–1996 collider run.
             We observe 39 t¯t candidate events in the dilepton and
             lepton+jets decay channels with an expected background of
             13.7 ± 2.2 events. For a top quark mass of 173.3 GeV/c2, we
             measure the t¯t production cross section to be 5.5 ± 1.8
             pb. © 1997 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.79.1203},
   Key = {Abachi97b}
}

@article{fds308223,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Alves, GA and Amos, N and Anderson,
             EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov,
             VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del-Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland,
             T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {Measurement of the top quark pair production cross section
             in the all-jets decay channel},
   Journal = {Physical Review Letters},
   Volume = {83},
   Number = {10},
   Pages = {1908-1913},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.83.1908},
   Abstract = {We present a measurement of t¯t production in p¯p
             collisions at √s = 1.8TeV from 110pb-1 of data collected
             in the all-jets decay channel with the D0 detector at
             Fermilab. A neural network analysis yields a cross section
             of 7.1 ± 2.8(stat) ± 1.5(syst)pb at a top quark mass (mt)
             of 172.1GeV/c2. Using previous D0 measurements from dilepton
             and single lepton channels, the combined D0 result for the
             t¯t production cross section is 5.9 ± 1.2(stat) ±
             1.1(syst)pb for mt = 172.1GeV/c2. © 1999 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.83.1908},
   Key = {fds308223}
}

@article{fds307766,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma,
             Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou,
             H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri,
             AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
             N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa,
             HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler,
             S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans,
             G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse,
             M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez,
             VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Measurement of the top quark pair production cross-section
             with ATLAS in the single lepton channel},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {711},
   Number = {3-4},
   Pages = {244-263},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.03.083},
   Abstract = {A measurement of the production cross-section for top quark
             pairs (tt-) in pp collisions at s=7TeV is presented using
             data recorded with the ATLAS detector at the Large Hadron
             Collider. Events are selected in the single lepton topology
             by requiring an electron or muon, large missing transverse
             momentum and at least three jets. With a data sample of 35
             pb -1, two different multivariate methods, one of which uses
             b-quark jet identification while the other does not, use
             kinematic variables to obtain cross-section measurements of
             σtt-=187±11(stat.)-17+18(syst.)±6(lumi.)pb and
             σtt-=173±17(stat.)-16+18(syst.)±6(lumi.)pb respectively.
             The two measurements are in agreement with each other and
             with QCD calculations. The first measurement has a better a
             priori sensitivity and constitutes the main result of this
             Letter. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.03.083},
   Key = {fds307766}
}

@article{fds308058,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the top-quark mass in all-hadronic decays in
             p anti-p collisions at CDF II},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {14},
   Pages = {142001},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.142001},
   Abstract = {We present a measurement of the top-quark mass Mtop in the
             all-hadronic decay channel t[overline t]-->W+bW-[overline
             b]-->q1[overline q]2bq3[overline q]4[overline b]. The
             analysis is performed using 310 pb-1 of sqrt(s)=1.96 TeV
             p[overline p] collisions collected with the CDF II detector
             using a multijet trigger. The mass measurement is based on
             an event-by-event likelihood which depends on both the
             sample purity and the value of the top-quark mass, using 90
             possible jet-to-parton assignments in the six-jet final
             state. The joint likelihood of 290 selected events yields a
             value of Mtop=177.1$\pm$4.9(stat)$\pm$4.7(syst)
             GeV/c2.},
   Doi = {10.1103/physrevlett.98.142001},
   Key = {fds308058}
}

@article{fds310349,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Measurement of the top-quark mass in the all-hadronic
             channel using the full CDF data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.091101},
   Abstract = {The top-quark mass Mtop is measured using top
             quark-antiquark pairs produced in proton-antiproton
             collisions at a center-of-mass energy of 1.96 TeV and that
             decay into a fully hadronic final state. The full data set
             collected with the CDF II detector at the Fermilab Tevatron
             Collider, corresponding to an integrated luminosity of
             9.3fb-1, is used. Events are selected that have six to eight
             jets, at least one of which is identified as having
             originated from a b quark. In addition, a multivariate
             algorithm, containing multiple kinematic variables as
             inputs, is used to discriminate signal events from
             background events due to QCD multijet production. Templates
             for the reconstructed top-quark mass are combined in a
             likelihood fit to measure Mtop with a simultaneous
             calibration of the jet energy scale. A value of
             Mtop=175.07±1.19(stat)-1.58+1.55(syst)GeV/c2 is obtained
             for the top-quark mass.},
   Doi = {10.1103/PhysRevD.90.091101},
   Key = {fds310349}
}

@article{fds310323,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Caughron, S and Cavaliere,
             V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin,
             V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro,
             A},
   Title = {Measurement of the top-quark mass in the fully hadronic
             decay channel from ATLAS data at [Formula: see
             text].},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {4},
   Pages = {158},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3373-1},
   Abstract = {The mass of the top quark is measured in a data set
             corresponding to 4.6 [Formula: see text] of proton-proton
             collisions with centre-of-mass energy [Formula: see
             text] TeV collected by the ATLAS detector at the LHC.
             Events consistent with hadronic decays of top-antitop quark
             pairs with at least six jets in the final state are
             selected. The substantial background from multijet
             production is modelled with data-driven methods that utilise
             the number of identified [Formula: see text]-quark jets and
             the transverse momentum of the sixth leading jet, which have
             minimal correlation. The top-quark mass is obtained from
             template fits to the ratio of three-jet to dijet mass. The
             three-jet mass is calculated from the three jets produced in
             a top-quark decay. Using these three jets the dijet mass is
             obtained from the two jets produced in the [Formula: see
             text] boson decay. The top-quark mass obtained from this fit
             is thus less sensitive to the uncertainty in the energy
             measurement of the jets. A binned likelihood fit yields a
             top-quark mass of [Formula: see text].},
   Doi = {10.1140/epjc/s10052-015-3373-1},
   Key = {fds310323}
}

@article{fds307870,
   Author = {Aaltonen, TEA},
   Title = {Measurement of the top-quark mass in the lepton+jets channel
             using a matrix element technique with the {CDF II}
             detector},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {7},
   Pages = {071105},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.071105},
   Abstract = {A measurement of the top-quark mass is presented using
             Tevatron data from proton-antiproton collisions at
             center-of-mass energy √s=1.96TeV collected with the CDF II
             detector. Events are selected from a sample of candidates
             for production of tt̄ pairs that decay into the lepton+jets
             channel. The top-quark mass is measured with an unbinned
             maximum likelihood method where the event probability
             density functions are calculated using signal and background
             matrix elements, as well as a set of parametrized
             jet-to-parton transfer functions. The likelihood function is
             maximized with respect to the top-quark mass, the signal
             fraction in the sample, and a correction to the jet energy
             scale (JES) calibration of the calorimeter jets. The
             simultaneous measurement of the JES correction (ΔJES)
             amounts to an additional in situ jet energy calibration
             based on the known mass of the hadronically decaying W
             boson. Using the data sample of 578 lepton+jets candidate
             events, corresponding to 3.2fb-1 of integrated luminosity,
             the top-quark mass is measured to be mt=172.4±1.4(stat+ΔJES)±1.
             3(syst)GeV/c2. © 2011 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.84.071105},
   Key = {fds307870}
}

@article{fds310270,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Measurement of the top-quark mass in the tt¯ dilepton
             channel using the full CDF Run II data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.032003},
   Abstract = {We present a measurement of the top-quark mass in events
             containing two leptons (electrons or muons) with a large
             transverse momentum, two or more energetic jets, and a
             transverse-momentum imbalance. We use the full
             proton-antiproton collision data set collected by the CDF
             experiment during the Fermilab Tevatron Run II at
             center-of-mass energy s=1.96 TeV, corresponding to an
             integrated luminosity of 9.1 fb-1. A special observable is
             exploited for an optimal reduction of the dominant
             systematic uncertainty, associated with the knowledge of the
             absolute energy of the hadronic jets. The distribution of
             this observable in the selected events is compared to
             simulated distributions of tt¯ dilepton signal and
             background. We measure a value for the top-quark mass of
             171.5±1.9 (stat)±2.5 (syst) GeV/c2.},
   Doi = {10.1103/PhysRevD.92.032003},
   Key = {fds310270}
}

@article{fds356565,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Akesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Bella,
             LA and Arabidze, G and Araque, JP and Araujo Ferraz,
             V},
   Title = {Measurement of the top-quark mass in tt¯ + 1-jet events
             collected with the ATLAS detector in pp collisions at √s =
             8 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {11},
   Year = {2019},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2019)150},
   Abstract = {A determination of the top-quark mass is presented using
             20.2 fb−1 of 8 TeV proton-proton collision data produced
             by the Large Hadron Collider and collected by the ATLAS
             experiment. The normalised differential cross section of
             top-quark pair production in association with an energetic
             jet is measured in the lepton+jets final state and unfolded
             to parton and particle levels. The unfolded distribution at
             parton level can be described using next-to-leading-order
             QCD predictions in terms of either the top-quark pole mass
             or the running mass as defined in the (modified) minimal
             subtraction scheme. A comparison between the experimental
             distribution and the theoretical prediction allows the
             top-quark mass to be extracted in the two schemes. The value
             obtained for the pole-mass scheme is: mtpole=171.1±0.4(stat)±0.9(syst)−0.3+0.7(theo)GeV
             The extracted value in the running-mass scheme is:
             mt(mt)=162.9±0.5(stat)±1.0(syst)−1.2+2.1(theo)GeV. The
             results for the top-quark mass using the two schemes are
             consistent, when translated from one scheme to the other.
             [Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP11(2019)150},
   Key = {fds356565}
}

@article{fds308063,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the top-quark mass using missing $E_T$ + jets
             events with secondary vertex $b-$tagging at CDF
             II},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {11},
   Pages = {111103},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.111103},
   Abstract = {We present a measurement of the top-quark mass in p[overline
             p] collisions at sqrt(s)=1.96 TeV which uses events with an
             inclusive signature of missing transverse energy and jets.
             The event selection is sensitive to t[overline
             t]-->W+bW-[overline b]-->lnubqq[prime][overline b]
             independent of the lepton flavor and results in a large
             acceptance for W-->taunu decays. All-hadronic t[overline t]
             decays and events with identified electrons or muons are
             vetoed to provide a statistically independent sample with
             respect to all previous measurements. The top-quark mass is
             inferred from the distribution of the scalar sum of all jet
             transverse energies and the missing transverse energy. Using
             311 pb-1 of integrated luminosity recorded by the Collider
             Detector at Fermilab, we measure a top-quark mass
             mt=172.3-9.6+10.8(stat)$\pm$10.8(syst) GeV/c2. While the
             uncertainty on mt is larger than that of other measurements,
             the result is statistically uncorrelated with those of other
             methods and thus can help to reduce the overall mt
             uncertainty when combined with other existing
             measurements.},
   Doi = {10.1103/PhysRevD.75.111103},
   Key = {fds308063}
}

@article{fds307954,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the Top-Quark Mass with Dilepton Events
             Selected Using Neuroevolution at CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {15},
   Pages = {152001},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.152001},
   Abstract = {We present an analysis of the mass of the X(3872)
             reconstructed via its decay to J/ψπ+π- using
             2.4  fb-1 of integrated luminosity from pp̅ collisions
             at sqrt[s]=1.96  TeV, collected with the CDF II detector
             at the Fermilab Tevatron. The possible existence of two
             nearby mass states is investigated. Within the limits of our
             experimental resolution the data are consistent with a
             single state, and having no evidence for two states we set
             upper limits on the mass difference between two hypothetical
             states for different assumed ratios of contributions to the
             observed peak. For equal contributions, the 95% confidence
             level upper limit on the mass difference is 3.6  MeV/c2.
             Under the single-state model the X(3872) mass is measured to
             be 3871.61$\pm$0.16(stat)$\pm$0.19(syst)  MeV/c2, which
             is the most precise determination to date.},
   Doi = {10.1103/physrevlett.102.152001},
   Key = {fds307954}
}

@article{fds307563,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Measurement of the top-quark pair-production cross section
             in events with two leptons and bottom-quark jets using the
             full CDF data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.091103},
   Abstract = {We present a measurement of the top-quark pair production
             cross section in proton-antiproton collisions at √s=1.96
             TeV. The data were collected at the Fermilab Tevatron by the
             CDF II detector and correspond to an integrated luminosity
             of 8.8 fb-1, representing the complete CDF Run II data set.
             We select events consistent with the production of top-quark
             pairs by requiring the presence of two reconstructed
             leptons, an imbalance in the total event transverse
             momentum, and jets. At least one jet is required to be
             identified as consistent with the fragmentation of a bottom
             quark using a secondary-vertex-finding algorithm. The 246
             candidate events are estimated to have a signal purity of
             91%. We measure a cross section of σ tt̄=7.09±0.84 pb,
             assuming a top-quark mass of 172.5 GeV/c2. The results are
             consistent with the standard model as predicted by
             next-to-leading-order calculations. Published by the
             American Physical Society.},
   Doi = {10.1103/PhysRevD.88.091103},
   Key = {fds307563}
}

@article{fds371119,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam
             Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral
             Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
             Ferraz, V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
             JF},
   Title = {Measurement of the total cross section and ρ -parameter
             from elastic scattering in pp collisions at √s=13 TeV with
             the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {5},
   Year = {2023},
   Month = {May},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11436-8},
   Abstract = {In a special run of the LHC with β⋆= 2.5 km,
             proton–proton elastic-scattering events were recorded at
             s=13 TeV with an integrated luminosity of 340μb-1 using the
             ALFA subdetector of ATLAS in 2016. The elastic cross section
             was measured differentially in the Mandelstam t variable in
             the range from - t= 2.5 · 10 - 4 GeV 2 to - t= 0.46 GeV 2
             using 6.9 million elastic-scattering candidates. This paper
             presents measurements of the total cross section σtot ,
             parameters of the nuclear slope, and the ρ -parameter
             defined as the ratio of the real part to the imaginary part
             of the elastic-scattering amplitude in the limit t→ 0 .
             These parameters are determined from a fit to the
             differential elastic cross section using the optical theorem
             and different parameterizations of the t-dependence. The
             results for σtot and ρ are σtot(pp→X)=104.7±1.1mb,ρ=0.098±0.011.
             The uncertainty in σtot is dominated by the luminosity
             measurement, and in ρ by imperfect knowledge of the
             detector alignment and by modelling of the nuclear
             amplitude.},
   Doi = {10.1140/epjc/s10052-023-11436-8},
   Key = {fds371119}
}

@article{fds313586,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurement of the total cross section from elastic
             scattering in pp collisions at √s=7 TeV with the ATLAS
             detector},
   Journal = {Nuclear Physics B},
   Volume = {889},
   Pages = {486-548},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {December},
   ISSN = {0550-3213},
   url = {http://dx.doi.org/10.1016/j.nuclphysb.2014.10.019},
   Abstract = {A measurement of the total pp cross section at the LHC at
             s=7 TeV is presented. In a special run with high-β⋆ beam
             optics, an integrated luminosity of 80 μb−1 was
             accumulated in order to measure the differential elastic
             cross section as a function of the Mandelstam momentum
             transfer variable t. The measurement is performed with the
             ALFA sub-detector of ATLAS. Using a fit to the differential
             elastic cross section in the |t| range from 0.01 GeV2 to 0.1
             GeV2 to extrapolate to |t|→0, the total cross section,
             σtot(pp→X), is measured via the optical theorem to be:
             σtot(pp→X)=95.35±0.38(stat.)±1.25(exp.)±0.37(extr.)mb,
             where the first error is statistical, the second accounts
             for all experimental systematic uncertainties and the last
             is related to uncertainties in the extrapolation to |t|→0.
             In addition, the slope of the elastic cross section at small
             |t| is determined to be B=19.73±0.14(stat.)±0.26(syst.)
             GeV−2.},
   Doi = {10.1016/j.nuclphysb.2014.10.019},
   Key = {fds313586}
}

@article{fds321082,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Measurement of the total cross section from elastic
             scattering in pp collisions at √s=8 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {761},
   Pages = {158-178},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.08.020},
   Abstract = {A measurement of the total pp cross section at the LHC at
             s=8 TeV is presented. An integrated luminosity of 500
             μb−1 was accumulated in a special run with high-β⋆
             beam optics to measure the differential elastic cross
             section as a function of the Mandelstam momentum transfer
             variable t. The measurement is performed with the ALFA
             sub-detector of ATLAS. Using a fit to the differential
             elastic cross section in the −t range from 0.014 GeV2 to
             0.1 GeV2 to extrapolate t→0, the total cross section,
             σtot(pp→X), is measured via the optical theorem to be
             σtot(pp→X)=96.07±0.18(stat.)±0.85(exp.)±0.31(extr.)mb,
             where the first error is statistical, the second accounts
             for all experimental systematic uncertainties and the last
             is related to uncertainties in the extrapolation t→0. In
             addition, the slope of the exponential function describing
             the elastic cross section at small t is determined to be
             B=19.74±0.05(stat.)±0.23(syst.)GeV−2.},
   Doi = {10.1016/j.physletb.2016.08.020},
   Key = {fds321082}
}

@article{fds316853,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
   Title = {Measurement of the transverse momentum and [Formula: see
             text] distributions of Drell-Yan lepton pairs in
             proton-proton collisions at [Formula: see text] TeV with
             the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {291},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4070-4},
   Abstract = {Distributions of transverse momentum [Formula: see text] and
             the related angular variable [Formula: see text] of
             DrellΓÇôYan lepton pairs are measured in
             20.3 fb[Formula: see text] of proton–proton
             collisions at [Formula: see text] TeV with the ATLAS
             detector at the LHC. Measurements in electron-pair and
             muon-pair final states are corrected for detector effects
             and combined. Compared to previous measurements in
             protonΓÇôproton collisions at [Formula: see
             text] TeV, these new measurements benefit from a larger
             data sample and improved control of systematic
             uncertainties. Measurements are performed in bins of
             lepton-pair mass above, around and below the <i>Z</i>-boson
             mass peak. The data are compared to predictions from
             perturbative and resummed QCD calculations. For values of
             [Formula: see text] the predictions from the Monte Carlo
             generator ResBos are generally consistent with the data
             within the theoretical uncertainties. However, at larger
             values of [Formula: see text] this is not the case. Monte
             Carlo generators based on the parton-shower approach are
             unable to describe the data over the full range of [Formula:
             see text] while the fixed-order prediction of Dynnlo falls
             below the data at high values of [Formula: see text]. ResBos
             and the parton-shower Monte Carlo generators provide a much
             better description of the evolution of the [Formula: see
             text] and [Formula: see text] distributions as a function of
             lepton-pair mass and rapidity than the basic shape of the
             data.},
   Doi = {10.1140/epjc/s10052-016-4070-4},
   Key = {fds316853}
}

@article{fds351090,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler,
             A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso,
             S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Araque, JP and Ferraz, VA and Pereira, RA and Arcangeletti, C},
   Title = {Measurement of the transverse momentum distribution of
             Drell–Yan lepton pairs in proton–proton collisions at
             √s=13 TeV with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {7},
   Year = {2020},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-8001-z},
   Abstract = {This paper describes precision measurements of the
             transverse momentum pTℓℓ (ℓ= e, μ) and of the angular
             variable ϕη∗ distributions of Drell–Yan lepton pairs
             in a mass range of 66–116 GeV. The analysis uses data
             from 36.1 fb- 1 of proton–proton collisions at a
             centre-of-mass energy of s=13TeV collected by the ATLAS
             experiment at the LHC in 2015 and 2016. Measurements in
             electron-pair and muon-pair final states are performed in
             the same fiducial volumes, corrected for detector effects,
             and combined. Compared to previous measurements in
             proton–proton collisions at s=7 and 8TeV, these new
             measurements probe perturbative QCD at a higher
             centre-of-mass energy with a different composition of
             initial states. They reach a precision of 0.2% for the
             normalized spectra at low values of pTℓℓ. The data are
             compared with different QCD predictions, where it is found
             that predictions based on resummation approaches can
             describe the full spectrum within uncertainties.},
   Doi = {10.1140/epjc/s10052-020-8001-z},
   Key = {fds351090}
}

@article{fds307758,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the transverse momentum distribution of W
             bosons in pp collisions at √s=7TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012005},
   Abstract = {This paper describes a measurement of the W boson transverse
             momentum distribution using ATLAS pp collision data from the
             2010 run of the LHC at √s=7TeV, corresponding to an
             integrated luminosity of about 31pb -1. Events form both
             W→eν and W→μν are used, and the transverse momentum
             of the W candidates is measured through the energy
             deposition in the calorimeter from the recoil of the W. The
             resulting distributions are unfolded to obtain the
             normalized differential cross sections as a function of the
             W boson transverse momentum. We present results for
             pTW<300GeV in the electron and muon channels as well as for
             their combination, and compare the combined results to the
             predictions of perturbative QCD and a selection of event
             generators. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.85.012005},
   Key = {fds307758}
}

@article{fds307861,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Measurement of the transverse momentum distribution of
             Z/γ* bosons in proton-proton collisions at s=7
             TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {5},
   Pages = {415-434},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.10.018},
   Abstract = {A measurement of the Z/γ* transverse momentum (pTZ)
             distribution in proton-proton collisions at s=7 TeV is
             presented using Z/γ*→e+e- and Z/γ*→μ+μ- decays
             collected with the ATLAS detector in data sets with
             integrated luminosities of 35 pb-1 and 40 pb-1,
             respectively. The normalized differential cross sections are
             measured separately for electron and muon decay channels as
             well as for their combination up to pTZ of 350 GeV for
             invariant dilepton masses 66 GeV<mℓℓ<116 GeV. The
             measurement is compared to predictions of perturbative QCD
             and various event generators. The prediction of resummed QCD
             combined with fixed order perturbative QCD is found to be in
             good agreement with the data. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.10.018},
   Key = {fds307861}
}

@article{fds310304,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Measurement of the transverse polarization of Λ and Λ ¯
             hyperons produced in proton-proton collisions at √s = 7
             TeV using the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.032004},
   Abstract = {The transverse polarization of Λ and Λ¯ hyperons produced
             in proton-proton collisions at a center-of-mass energy of 7
             TeV is measured. The analysis uses 760 μb-1 of minimum bias
             data collected by the ATLAS detector at the LHC in the year
             2010. The measured transverse polarization averaged over
             Feynman xF from 5×10-5 to 0.01 and transverse momentum pT
             from 0.8 to 15 GeV is -0.010±0.005(stat)±0.004(syst) for
             Λ and 0.002±0.006(stat)±0.004(syst) for Λ¯. It is also
             measured as a function of xF and pT, but no significant
             dependence on these variables is observed. Prior to this
             measurement, the polarization was measured at fixed-target
             experiments with center-of-mass energies up to about 40 GeV.
             The ATLAS results are compatible with the extrapolation of a
             fit from previous measurements to the xF range covered by
             this measurement.},
   Doi = {10.1103/PhysRevD.91.032004},
   Key = {fds310304}
}

@article{fds375335,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Aktas, S and Al Khoury and K and Alberghi,
             GL and Albert, J and Albicocco, P and Albouy, GL and Alderweireldt, S and Alegria, ZL and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
             Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
             C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
             M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
             SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
   Title = {Measurement of the tt¯ cross section and its ratio to the Z
             production cross section using pp collisions at s=13.6 TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {848},
   Pages = {138376-138376},
   Publisher = {Elsevier BV},
   Year = {2024},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.138376},
   Abstract = {The inclusive top-quark-pair production cross section σtt¯
             and its ratio to the Z-boson production cross section have
             been measured in proton–proton collisions at s=13.6 TeV,
             using 29 fb−1 of data collected in 2022 with the ATLAS
             experiment at the Large Hadron Collider. Using events with
             an opposite-charge electron-muon pair and b-tagged jets, and
             assuming Standard Model decays, the top-quark-pair
             production cross section is measured to be
             σtt¯=850±3(stat.)±18(syst.)±20(lumi.) pb. The ratio of
             the tt¯ and the Z-boson production cross sections is also
             measured, where the Z-boson contribution is determined for
             inclusive e+e− and μ+μ− events in a fiducial phase
             space. The relative uncertainty on the ratio is reduced
             compared to the tt¯ cross section, thanks to the
             cancellation of several systematic uncertainties. The result
             for the ratio, Rtt¯/Z=1.145±0.003(stat.)±0.021(syst.)±0.002(lumi.)
             is consistent with the Standard Model prediction using the
             PDF4LHC21 PDF set.},
   Doi = {10.1016/j.physletb.2023.138376},
   Key = {fds375335}
}

@article{fds350336,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Araque, JP and Ferraz, VA and Pereira,
             RA},
   Title = {Measurement of the tt¯ production cross-section and lepton
             differential distributions in eμ dilepton events from pp
             collisions at √s=13TeV with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {6},
   Year = {2020},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-7907-9},
   Abstract = {The inclusive top quark pair (tt¯) production cross-section
             σtt¯ has been measured in proton–proton collisions at
             s=13TeV, using 36.1 fb- 1 of data collected in 2015–2016
             by the ATLAS experiment at the LHC. Using events with an
             opposite-charge eμ pair and b-tagged jets, the
             cross-section is measured to be: σtt¯=826.4±3.6(stat)±11.5(syst)±15.7(lumi)±1.9(beam)pb,where
             the uncertainties reflect the limited size of the data
             sample, experimental and theoretical systematic effects, the
             integrated luminosity, and the LHC beam energy, giving a
             total uncertainty of 2.4%. The result is consistent with
             theoretical QCD calculations at next-to-next-to-leading
             order. It is used to determine the top quark pole mass via
             the dependence of the predicted cross-section on mtpole,
             giving mtpole=173.1-2.1+2.0GeV. It is also combined with
             measurements at s=7TeV and s=8TeV to derive ratios and
             double ratios of tt¯ and Z cross-sections at different
             energies. The same event sample is used to measure absolute
             and normalised differential cross-sections as functions of
             single-lepton and dilepton kinematic variables, and the
             results are compared with predictions from various Monte
             Carlo event generators.},
   Doi = {10.1140/epjc/s10052-020-7907-9},
   Key = {fds350336}
}

@article{fds310328,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the tt¯ production cross-section as a
             function of jet multiplicity and jet transverse momentum in
             7 TeV proton-proton collisions with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2015)020},
   Abstract = {Abstract: The tt¯$$ t\overline{t} $$ production
             cross-section dependence on jet multiplicity and jet
             transverse momentum is reported for proton-proton collisions
             at a centre-of-mass energy of 7 TeV in the single-lepton
             channel. The data were collected with the ATLAS detector at
             the CERN Large Hadron Collider and comprise the full 2011
             data sample corresponding to an integrated luminosity of 4.6
             fb−1. Differential cross-sections are presented as a
             function of the jet multiplicity for up to eight jets using
             jet transverse momentum thresholds of 25, 40, 60, and 80
             GeV, and as a function of jet transverse momentum up to the
             fifth jet. The results are shown after background
             subtraction and corrections for all known detector effects,
             within a kinematic range closely matched to the experimental
             acceptance. Several QCD-based Monte Carlo models are
             compared with the results. Sensitivity to the parton shower
             modelling is found at the higher jet multiplicities, at high
             transverse momentum of the leading jet and in the transverse
             momentum spectrum of the fifth leading jet. The
             MC@NLO+HERWIG MC is found to predict too few events at
             higher jet multiplicities.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP01(2015)020},
   Key = {fds310328}
}

@article{fds352890,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {Measurement of the tt¯ production cross-section in the
             lepton+jets channel at s=13 TeV with the ATLAS
             experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {810},
   Year = {2020},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2020.135797},
   Abstract = {The top anti-top quark production cross-section is measured
             in the lepton+jets channel using proton–proton collision
             data at a centre-of-mass energy of s=13 TeV collected with
             the ATLAS detector at the LHC. The dataset corresponds to an
             integrated luminosity of 139 fb−1. Events with exactly one
             charged lepton and four or more jets in the final state,
             with at least one jet containing b-hadrons, are used to
             determine the tt¯ production cross-section through a
             profile-likelihood fit. The inclusive cross-section is
             measured to be σinc=830±0.4(stat.)±36(syst.)±14(lumi.)pb
             with a relative uncertainty of 4.6%. The result is
             consistent with theoretical calculations at
             next-to-next-to-leading order in perturbative QCD. The
             fiducial tt¯ cross-section within the experimental
             acceptance is also measured.},
   Doi = {10.1016/j.physletb.2020.135797},
   Key = {fds352890}
}

@article{fds321132,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of the tt¯ production cross-section using eμ
             events with b-tagged jets in pp collisions at √s=13TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {761},
   Pages = {136-157},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.08.019},
   Abstract = {This paper describes a measurement of the inclusive top
             quark pair production cross-section (σtt¯) with a data
             sample of 3.2fb−1 of proton–proton collisions at a
             centre-of-mass energy of s=13TeV, collected in 2015 by the
             ATLAS detector at the LHC. This measurement uses events with
             an opposite-charge electron–muon pair in the final state.
             Jets containing b-quarks are tagged using an algorithm based
             on track impact parameters and reconstructed secondary
             vertices. The numbers of events with exactly one and exactly
             two b-tagged jets are counted and used to determine
             simultaneously σtt¯ and the efficiency to reconstruct and
             b-tag a jet from a top quark decay, thereby minimising the
             associated systematic uncertainties. The cross-section is
             measured to be: σtt¯=818±8(stat)±27(syst)±19(lumi)±12(beam)
             pb, where the four uncertainties arise from data statistics,
             experimental and theoretical systematic effects, the
             integrated luminosity and the LHC beam energy, giving a
             total relative uncertainty of 4.4%. The result is consistent
             with theoretical QCD calculations at next-to-next-to-leading
             order. A fiducial measurement corresponding to the
             experimental acceptance of the leptons is also
             presented.},
   Doi = {10.1016/j.physletb.2016.08.019},
   Key = {fds321132}
}

@article{fds356726,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Measurement of the tt¯ γ production cross section in
             proton-proton collisions at √s=8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {11},
   Year = {2017},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2017)086},
   Abstract = {The cross section of a top-quark pair produced in
             association with a photon is measured in proton-proton
             collisions at a centre-of-mass energy of s=8 TeV with 20.2
             fb−1 of data collected by the ATLAS detector at the Large
             Hadron Collider in 2012. The measurement is performed by
             selecting events that contain a photon with transverse
             momentum pT > 15 GeV, an isolated lepton with large
             transverse momentum, large missing transverse momentum, and
             at least four jets, where at least one is identified as
             originating from a b-quark. The production cross section is
             measured in a fiducial region close to the selection
             requirements. It is found to be 139 ± 7 (stat.) ± 17
             (syst.) fb, in good agreement with the theoretical
             prediction at next-to-leading order of 151 ± 24 fb. In
             addition, differential cross sections in the fiducial region
             are measured as a function of the transverse momentum and
             pseudorapidity of the photon.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP11(2017)086},
   Key = {fds356726}
}

@article{fds356608,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA},
   Title = {Measurement of the tt¯Z and tt¯W cross sections in
             proton-proton collisions at s=13 TeV with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {99},
   Number = {7},
   Year = {2019},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.99.072009},
   Abstract = {A measurement of the associated production of a top-quark
             pair (tt) with a vector boson (W, Z) in proton-proton
             collisions at a center-of-mass energy of 13 TeV is
             presented, using 36.1 fb-1 of integrated luminosity
             collected by the ATLAS detector at the Large Hadron
             Collider. Events are selected in channels with two same- or
             opposite-sign leptons (electrons or muons), three leptons or
             four leptons, and each channel is further divided into
             multiple regions to maximize the sensitivity of the
             measurement. The ttZ and ttW production cross sections are
             simultaneously measured using a combined fit to all regions.
             The best-fit values of the production cross sections are
             σttZ=0.95±0.08stat±0.10syst pb and σttW=0.87±0.13stat±0.14syst
             pb in agreement with the Standard Model predictions. The
             measurement of the ttZ cross section is used to set
             constraints on effective field theory operators which modify
             the ttZ vertex.},
   Doi = {10.1103/PhysRevD.99.072009},
   Key = {fds356608}
}

@article{fds313578,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canelli, F and Canepa, A and Casarsa, M and Carlsmith, D and Carosi,
             R and Carron, S and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             I and Cho, K and Chokheli, D and Chou, JP and Chuang, S and Chung, K and Chung, WH and Chung, YS and Cijliak, M and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Cruz, A and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Demers,
             S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and Dituro, P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
             JP and Field, RD and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii,
             Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
             M and Grosso-Pilcher, C and Grundler, U and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
             M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
             AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev,
             DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca, G and Margaroli, and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic,
             N and Miles, J and Miller, L and Miller, R and Miller, JS and Mills, C and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi,
             N and Mohr, B and Moore, R and Morello, M and Fernandez, PAM and Muelmenstaedt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Nelson, T and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa, T and Oh, SH and Oh, YD and Ohsugi,
             T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Osterberg,
             K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou,
             V and Paramonov, AA and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo,
             T and Rolli, S and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis,
             RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sill, A and Sinervo, P and Sisakyan, A and Sjolin, J and Skiba, A and Slaughter, AJ and Sliwa,
             K},
   Title = {Measurement of the tt̄ production cross section in pp̄
             collisions at s=1.96 TeV using lepton plus jets events with
             semileptonic B decays to muons},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {72},
   Number = {3},
   Pages = {1-20},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   ISSN = {1550-7998},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000231564900007&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Abstract = {We present a measurement of the tt̄ production cross
             section using 194 pb-1 of CDF II data using events with a
             high transverse momentum electron or muon, three or more
             jets, and missing transverse energy. The measurement assumes
             100% t→Wb branching fraction. Events consistent with tt̄
             decay are found by identifying jets containing heavy-flavor
             semileptonic decays to muons. The dominant backgrounds are
             evaluated directly from the data. Based on 20 candidate
             events and an expected background of 9.5±1.1 events, we
             measure a production cross section of 5.3±3.3-1.0+1.3 pb,
             in agreement with the standard model. © 2005 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.72.032002},
   Key = {fds313578}
}

@article{fds308147,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery,
             M},
   Title = {Measurement of the tt̄ production cross section in pp̄
             collisions at √s = 1.96 TeV using lepton + jets events
             with secondary vertex b -tagging},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {5},
   Pages = {1-28},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.052003},
   Abstract = {We present a measurement of the tt̄ production cross
             section using events with one charged lepton and jets from
             pp̄ collisions at a center-of-mass energy of 1.96 TeV. In
             these events, heavy flavor quarks from top quark decay are
             identified with a secondary vertex tagging algorithm. From
             162 pb<sup>-1</sup> of data collected by the Collider
             Detector at Fermilab, a total of 48 candidate events are
             selected, where 13.5 ± 1.8 events are expected from
             background contributions. We measure a tt̄ production cross
             section of 5.6<inf>-1.1</inf><sup>+1.2</sup>(stat.)<inf>-0.6</inf><sup>+0.9</sup>(syst.)
             pb. © 2005 The American Physical Society.},
   Doi = {10.1103/PhysRevD.71.052003},
   Key = {fds308147}
}

@article{fds313580,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura, P and Campanelli,
             M and Campbell, M and Canepa, A and Casarsa, M and Carlsmith, D and Carron,
             S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen,
             C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang,
             S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker,
             GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
             JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
             J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
             N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, J and Frisch,
             H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti,
             P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
             M and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
             M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
             H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko,
             S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko,
             I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann,
             SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefevre, R and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson,
             M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel,
             P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
             B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller,
             T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu,
             C and Neubauer, MS and Newman-Holmes, C and Nicollerat, AS and Nigmanov,
             T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh,
             SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
             C and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn,
             F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray,
             H and Reichold, A and Reisert, B and Rekovic, V and Renton, P and Rescigno,
             M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shochet,
             M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba,
             A},
   Title = {Measurement of the tt̄ production cross section in pp̄
             collisions at √s=1:96 TeV using kinematic fitting of
             b-tagged lepton+jet events},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {7},
   Pages = {1-11},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   ISSN = {1550-7998},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000228765400011&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Abstract = {We report a measurement of the tt̄ production cross section
             using the CDF II detector at the Fermilab Tevatron. The data
             consist of events with an energetic electron or muon,
             missing transverse energy, and three or more hadronic jets,
             at least one of which is identified as a b-quark jet by
             reconstructing a secondary vertex. The background fraction
             is determined from a fit of the transverse energy of the
             leading jet. Using 162 ± 10 pb -1 of data, the total cross
             section is found to be 6.0 ± 1.6(stat.) ± 1.2(syst.) pb,
             which is consistent with the standard model prediction. ©
             2005 The American Physical Society.},
   Doi = {10.1103/PhysRevD.71.072005},
   Key = {fds313580}
}

@article{fds307991,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the tt̅ cross section in pp̅ collisions at
             sqrt[s] =1.96 TeV using dilepton events with a lepton plus
             track selection},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {11},
   Pages = {112007},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.112007},
   Abstract = {This paper reports a measurement of the cross section for
             the pair production of top quarks in pp̅ collisions at
             sqrt[s]=1.96  TeV at the Fermilab Tevatron. The data
             were collected from the CDF run II detector in a set of runs
             with a total integrated luminosity of 1.1  fb-1. The
             cross section is measured in the dilepton channel, the
             subset of tt̅ events in which both top quarks decay through
             t→Wb→ℓνb, where ℓ=e, μ, or τ. The lepton pair is
             reconstructed as one identified electron or muon and one
             isolated track. The use of an isolated track to identify the
             second lepton increases the tt̅ acceptance, particularly
             for the case in which one W decays as W→τν. The purity
             of the sample may be further improved at the cost of a
             reduction in the number of signal events, by requiring an
             identified b jet. We present the results of measurements
             performed with and without the request of an identified b
             jet. The former is the first published CDF result for which
             a b-jet requirement is added to the dilepton selection. In
             the CDF data there are 129 pretag lepton+track candidate
             events, of which 69 are tagged. With the tagging
             information, the sample is divided into tagged and untagged
             subsamples, and a combined cross section is calculated by
             maximizing a likelihood. The result is σtt̅ =9.6 &plusmn;
             1.2(stat)-0.5+0.6(sys) &plusmn; 0.6(lum)  pb, assuming a
             branching ratio of BR(W→ℓν)=10.8% and a top mass of
             mt=175  GeV/c2.},
   Doi = {10.1103/PhysRevD.79.112007},
   Key = {fds307991}
}

@article{fds307982,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the t[overline t] production cross section in
             2 fb[sup -1] of p[overline p] collisions at sqrt(s) = 1.96
             TeV using lepton plus jets events with soft muon b
             tagging},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {5},
   Pages = {052007},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.052007},
   Abstract = {We present a measurement of the tt̄ production cross
             section in pp̄ collisions at s=1.96TeV using events
             containing a high transverse momentum electron or muon,
             three or more jets, and missing transverse energy. Events
             consistent with tt̄ decay are found by identifying jets
             containing candidate heavy-flavor semileptonic decays to
             muons. The measurement uses a CDF run II data sample
             corresponding to 2fb-1 of integrated luminosity. Based on
             248 candidate events with three or more jets and an expected
             background of 79.5±5.3 events, we measure a production
             cross section of 9.1±1.6pb. © 2009 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.79.052007},
   Key = {fds307982}
}

@article{fds310368,
   Author = {The ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
             J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa,
             C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung,
             C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso,
             S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Measurement of the underlying event in jet events from
             7 TeV proton–proton collisions with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {74},
   Number = {8},
   Pages = {1-29},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-2965-5},
   Abstract = {Distributions sensitive to the underlying event in QCD jet
             events have been measured with the ATLAS detector at the
             LHC, based on (Formula presented.) of proton–proton
             collision data collected at a centre-of-mass energy of
             7 (Formula presented.). Charged-particle mean (Formula
             presented.) and densities of all-particle (Formula
             presented.) and charged-particle multiplicity and (Formula
             presented.) have been measured in regions azimuthally
             transverse to the hardest jet in each event. These are
             presented both as one-dimensional distributions and with
             their mean values as functions of the leading-jet transverse
             momentum from 20 to 800 (Formula presented.). The
             correlation of charged-particle mean (Formula presented.)
             with charged-particle multiplicity is also studied, and the
             (Formula presented.) densities include the forward rapidity
             region; these features provide extra data constraints for
             Monte Carlo modelling of colour reconnection and
             beam-remnant effects respectively. For the first time,
             underlying event observables have been computed separately
             for inclusive jet and exclusive dijet event selections,
             allowing more detailed study of the interplay of multiple
             partonic scattering and QCD radiation contributions to the
             underlying event. Comparisons to the predictions of
             different Monte Carlo models show a need for further model
             tuning, but the standard approach is found to generally
             reproduce the features of the underlying event in both types
             of event selection.},
   Doi = {10.1140/epjc/s10052-014-2965-5},
   Key = {fds310368}
}

@article{fds307765,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni, G},
   Title = {Measurement of the W ±Z production cross section
             and limits on anomalous triple gauge couplings in
             proton-proton collisions at s=7 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {709},
   Number = {4-5},
   Pages = {341-357},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.053},
   Abstract = {This Letter presents a measurement of W ±Z production in
             1.02 fb -1 of pp collision data at s=7 TeV collected by the
             ATLAS experiment in 2011. Doubly leptonic decay events are
             selected with electrons, muons and missing transverse
             momentum in the final state. In total 71 candidates are
             observed, with a background expectation of
             12.1±1.4(stat.)-2.0+4.1(syst.) events. The total cross
             section for W ±Z production for Z/γ * masses within the
             range 66 GeV to 116 GeV is determined to be
             σWZtot=20.5-2.8+3.1(stat.)-1.3+1.4(syst.)-0.8+0.9(lumi.)
             pb, which is consistent with the Standard Model expectation
             of 17.30.8+1.3 pb. Limits on anomalous triple gauge boson
             couplings are extracted. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.02.053},
   Key = {fds307765}
}

@booklet{Abbott98a,
   Author = {B. Abbott and M. Abolins and B. S. Acharya and I. Adam and D. L. Adams and M. Adams and S. Ahn and H. Aihara and G. A.
             Alves and N. Amos and E. W. Anderson and R. Astur and M. M.
             Baarmand and A. Baden and V. Balamurali and J. Balderston and B. Baldin and},
   Title = {Measurement of the W boson mass},
   Journal = {Physical Review D},
   Volume = {5809},
   Number = {9},
   Pages = {art. no. -- 092003},
   Year = {1998},
   Month = {November},
   Key = {Abbott98a}
}

@article{fds308238,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
             EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis,
             E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram,
             I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {Measurement of the W boson mass},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {58},
   Number = {9},
   Pages = {920031-9200337},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.58.092003},
   Abstract = {We present a measurement of the W boson mass using data
             collected by the D0 experiment at the Fermilab Tevatron
             during 1994–1995. We identify W bosons by their decays to
             [Formula Presented] final states. We extract the W mass
             [Formula Presented] by fitting the transverse mass and
             transverse electron momentum spectra from a sample of 28 323
             [Formula Presented] decay candidates. We use a sample of
             3563 dielectron events, mostly due to [Formula Presented]
             decays, to constrain our model of the detector response.
             From the transverse mass fit we measure [Formula Presented]
             GeV. Combining this with our previously published result
             from data taken in 1992–1993, we obtain [Formula
             Presented]. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.58.092003},
   Key = {fds308238}
}

@article{fds308046,
   Author = {Kotwal, AV and Stark, J},
   Title = {Measurement of the W boson mass at the Tevatron},
   Journal = {Annual Reviews of Nuclear and Particle Science},
   Volume = {58},
   Number = {1},
   Pages = {28},
   Publisher = {ANNUAL REVIEWS},
   Year = {2008},
   Month = {November},
   url = {http://dx.doi.org/10.1146/annurev.nucl.58.110707.171227},
   Abstract = {Over the past four decades, the standard model of
             electroweak interactions has achieved tremendous success in
             describing the experimental data. One of the key observables
             is the mass M w of the W boson. The experimental
             measurements, including M w, have reached a level of
             precision that tests the theory at the quantum loop level,
             providing indirect constraints on the hypothetical Higgs
             boson and other new physics. Improved measurements of M w
             are driven by new data from Run II of the Fermilab Tevatron
             (pp̄ collider at ̂s = 1.96 TeV). We discuss the techniques
             used for measuring M w at hadron colliders, summarize the
             measurements from Run I of the Tevatron, and review the
             state of the art of the Run II analyses, which are based on
             significantly larger data sets collected with upgraded
             detectors. We discuss the constraints on the Higgs boson,
             and conclude with a discussion of the ultimate precision in
             M w that can be expected from Run II. Copyright © 2008 by
             Annual Reviews. All rights reserved.},
   Doi = {10.1146/annurev.nucl.58.110707.171227},
   Key = {fds308046}
}

@article{fds308195,
   Author = {Song, XF and Sosebee, M and Sotnikova, N and Souza, M and Stanton, NR and Steinbruck, G and Stephens, RW and Stevenson, ML and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Streets, K and Strovink, M and Stutte, L and Sznajder, A and Tamburello, P and Tarazi,
             J and Tartaglia, M and Thomas, TL and Thompson, J and Toback, D and Trippe,
             TG and Turcot, AS and Tuts, PM},
   Title = {Measurement of the W boson mass using electrons at large
             rapidities},
   Journal = {Physical review letters},
   Volume = {84},
   Number = {2},
   Pages = {222-227},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.84.222},
   Abstract = {We report a measurement of the W boson mass based on an
             integrated luminosity of 82 pb(-1) from p&pmacr; collisions
             at sqrt[s] = 1.8 TeV recorded in 1994-1995 by the D0
             detector at the Fermilab Tevatron. We identify W bosons by
             their decays to enu, where the electron is detected in the
             forward calorimeters. We extract the mass by fitting the
             transverse mass and the electron and neutrino transverse
             momentum spectra of 11 089 W boson candidates. We measure
             M(W) = 80.691+/-0.227 GeV. By combining this measurement
             with our previously published central calorimeter results
             from data taken in 1992-1993 and 1994-1995, we obtain M(W) =
             80.482+/-0.091 GeV.},
   Doi = {10.1103/physrevlett.84.222},
   Key = {fds308195}
}

@article{fds308198,
   Author = {Abbott, B and al, E},
   Title = {Measurement of the W boson mass using large rapidity
             electrons},
   Journal = {Phys. Rev. D},
   Volume = {62},
   Number = {092006},
   Pages = {33},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.62.092006},
   Abstract = {We present a measurement of the W boson mass using data
             collected by the DØ experiment at the Fermilab Tevatron
             during 1994-1995. We identify W bosons by their decays to
             enu final states where the electron is detected in a forward
             calorimeter. We extract the W boson mass MW by fitting the
             transverse mass and transverse electron and neutrino
             momentum spectra from a sample of 11089 W->enu decay
             candidates. We use a sample of 1687 dielectron events,
             mostly due to Z->ee decays, to constrain our model of the
             detector response. Using the forward calorimeter data, we
             measure MW = 80.691±0.227 GeV.},
   Doi = {10.1103/PhysRevD.62.092006},
   Key = {fds308198}
}

@article{fds307783,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A},
   Title = {Measurement of the W boson polarization in top quark decays
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP06(2012)088},
   Abstract = {This paper presents measurements of the polarization ofW
             bosons in top quark decays, derived from tt̄ events with
             missing transverse momentum, one charged lepton and at least
             four jets, or two charged leptons and at least two jets.
             Data from pp collisions at a centre-of-mass energy of 7 TeV
             were collected with the ATLAS experiment at the LHC and
             correspond to an integrated luminosity of 1.04 fb-1. The
             measured fractions of longitudinally, left- and right-handed
             polarization are F0 = 0.67 ± 0.07, FL = 0.32 ± 0.04 and FR
             = 0.01 ± 0.05, in agreement with the Standard Model
             predictions. As the polarization of the W bosons in top
             quark decays is sensitive to the Wtb vertex Lorentz
             structure and couplings, the measurements were used to set
             limits on anomalous contributions to the Wtb couplings. ©
             CERN.},
   Doi = {10.1007/JHEP06(2012)088},
   Key = {fds307783}
}

@article{fds313618,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Measurement of the W W + W Z cross section and limits on
             anomalous triple gauge couplings using final states with one
             lepton, missing transverse momentum, and two jets with the
             ATLAS detector at √s = 7 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {1},
   Pages = {1-42},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2015)049},
   Abstract = {Abstract: The production of a W boson decaying to eν or
             μν in association with a W or Z boson decaying to two jets
             is studied using 4.6 fb−1 of proton-proton collision data
             at √s =7 TeV recorded with the ATLAS detector at the LHC.
             The combined WW + WZ cross section is measured with a
             significance of 3.4σ and is found to be 68±7 (stat.)±19
             (syst.) pb, in agreement with the Standard Model expectation
             of 61.1±2.2 pb. The distribution of the transverse momentum
             of the dijet system is used to set limits on anomalous
             contributions to the triple gauge coupling vertices and on
             parameters of an effective-field-theory model.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP01(2015)049},
   Key = {fds313618}
}

@article{fds307842,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak,
             MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Baltasar Dos Santos Pedrosa,
             F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon,
             P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch, V and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
             M and Benedict, BH and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci,
             F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Biesiada, J and Biglietti,
             M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel,
             A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Boonekamp, M and Boorman,
             G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boulahouache, C and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Brubaker, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse,
             M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camard,
             A and Camarri, P and Cambiaghi, M and Cameron, D and Cammin, J and Campana,
             S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
             J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Cazzato, A and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, L and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov,
             A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan,
             M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Measurement of the W+ W- cross section in sqrt(s) =
             7  TeV pp collisions with ATLAS.},
   Journal = {Physical review letters},
   Volume = {107},
   Number = {4},
   Pages = {041802},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.107.041802},
   Abstract = {This Letter presents a measurement of the W+ W- production
             cross section in sqrt(s) = 7  TeV pp collisions by the
             ATLAS experiment, using 34  pb(-1) of integrated
             luminosity produced by the Large Hadron Collider at CERN.
             Selecting events with two isolated leptons, each either an
             electron or a muon, 8 candidate events are observed with an
             expected background of 1.7 ± 0.6 events. The measured cross
             section is 41(-16)(+20)(stat) ± 5(syst)±1(lumi)  pb,
             which is consistent with the standard model prediction of 44
             ± 3  pb calculated at next-to-leading order in
             QCD.},
   Doi = {10.1103/physrevlett.107.041802},
   Key = {fds307842}
}

@article{fds356730,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of the W+W production
             cross section in pp collisions at a centre-of-mass energy of
             √s = 13 TeV with the ATLAS experiments},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {773},
   Pages = {354-374},
   Year = {2017},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2017.08.047},
   Abstract = {The production of opposite-charge W-boson pairs in
             proton–proton collisions at s=13 TeV is measured using
             data corresponding to 3.16 fb−1 of integrated luminosity
             collected by the ATLAS detector at the CERN Large Hadron
             Collider in 2015. Candidate W-boson pairs are selected by
             identifying their leptonic decays into an electron, a muon
             and neutrinos. Events with reconstructed jets are not
             included in the candidate event sample. The cross-section
             measurement is performed in a fiducial phase space close to
             the experimental acceptance and is compared to theoretical
             predictions. Agreement is found between the measurement and
             the most accurate calculations available.},
   Doi = {10.1016/j.physletb.2017.08.047},
   Key = {fds356730}
}

@article{fds321134,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of the W±Z boson pair-production
             cross section in pp collisions at s=13 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {762},
   Pages = {1-22},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.08.052},
   Abstract = {The production of W±Z events in proton–proton collisions
             at a centre-of-mass energy of 13 TeV is measured with the
             ATLAS detector at the LHC. The collected data correspond to
             an integrated luminosity of 3.2 fb−1. The W±Z candidates
             are reconstructed using leptonic decays of the gauge bosons
             into electrons or muons. The measured inclusive cross
             section in the detector fiducial region for leptonic decay
             modes is σW±Z→ℓ′νℓℓfid.=63.2±3.2(stat.)±2.6(sys.)±1.5(lumi.)
             fb. In comparison, the next-to-leading-order Standard Model
             prediction is 53.4−2.8+3.6 fb. The extrapolation of the
             measurement from the fiducial to the total phase space
             yields σW±Ztot.=50.6±2.6(stat.)±2.0(sys.)±0.9(th.)±1.2(lumi.)
             pb, in agreement with a recent next-to-next-to-leading-order
             calculation of 48.2−1.0+1.1 pb. The cross section as a
             function of jet multiplicity is also measured, together with
             the charge-dependent W+Z and W−Z cross sections and their
             ratio.},
   Doi = {10.1016/j.physletb.2016.08.052},
   Key = {fds321134}
}

@article{fds321103,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Measurement of the WW and WZ production cross section using
             final states with a charged lepton and heavy-flavor jets in
             the full CDF Run II data set},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.032008},
   Abstract = {We present a measurement of the total WW and WZ production
             cross sections in pp collision at s=1.96 TeV, in a final
             state consistent with leptonic W boson decay and jets
             originating from heavy-flavor quarks from either a W or a Z
             boson decay. This analysis uses the full data set collected
             with the CDF II detector during Run II of the Tevatron
             collider, corresponding to an integrated luminosity of 9.4
             fb-1. An analysis of the dijet mass spectrum provides 3.7σ
             evidence of the summed production processes of either WW or
             WZ bosons with a measured total cross section of
             σWW+WZ=13.7±3.9 pb. Independent measurements of the WW and
             WZ production cross sections are allowed by the different
             heavy-flavor decay patterns of the W and Z bosons and by the
             analysis of secondary-decay vertices reconstructed within
             heavy-flavor jets. The productions of WW and of WZ dibosons
             are independently seen with significances of 2.9σ and
             2.1σ, respectively, with total cross sections of
             σWW=9.4±4.2 pb and σWZ=3.7-2.2+2.5 pb. The measurements
             are consistent with standard-model predictions.},
   Doi = {10.1103/PhysRevD.94.032008},
   Key = {fds321103}
}

@article{fds307780,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
             JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
             Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro,
             NF and Cataldi, G and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung,
             SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC},
   Title = {Measurement of the WW cross section in √s=7 TeV pp
             collisions with the ATLAS detector and limits on anomalous
             gauge couplings},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {712},
   Number = {4-5},
   Pages = {289-308},
   Publisher = {Elsevier BV},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.05.003},
   Abstract = {This Letter reports a measurement of the WW production cross
             section in √s=7 TeV pp collisions using data corresponding
             to an integrated luminosity of 1.02 fb-1 collected with the
             ATLAS detector. Using leptonic decays of oppositely charged
             W bosons, the total measured cross section is
             σ(pp→WW)=54.4±4.0(stat.)±3.9(syst.)±2.0(lumi.) pb,
             consistent with the Standard Model prediction of
             σ(pp→WW)=44.4±2.8 pb. Limits on anomalous electroweak
             triple-gauge couplings are extracted from a fit to the
             transverse-momentum distribution of the leading charged
             lepton in the event. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.05.003},
   Key = {fds307780}
}

@article{fds307810,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'errico, M},
   Title = {Measurement of the WZ cross section and triple gauge
             couplings in pp̄ collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.031104},
   Abstract = {This article describes the current most precise measurement
             of the WZ production cross section as well as limits on
             anomalous WWZ couplings at a center-of-mass energy of 1.96
             TeV in proton-antiproton collisions for the Collider
             Detector at Fermilab (CDF). WZ candidates are reconstructed
             from decays containing three charged leptons and missing
             energy from a neutrino, where the charged leptons are either
             electrons or muons. Using data collected by the CDF II
             detector (7.1fb -1 of integrated luminosity), 63 candidate
             events are observed with the expected background
             contributing 8±1 events. The measured total cross section
             σ(pp̄→WZ)=3.93-0.53+0.60(stat)-0. 46+0.59(syst)pb is in
             good agreement with the standard model prediction of
             3.50±0.21. The same sample is used to set limits on
             anomalous WWZ couplings. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.86.031104},
   Key = {fds307810}
}

@article{fds307751,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the W→τντ cross section in pp
             collisions at s=7 TeV with the ATLAS experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {706},
   Number = {4-5},
   Pages = {276-294},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.11.057},
   Abstract = {The cross section for the production of W bosons with
             subsequent decay W→τντ is measured with the ATLAS
             detector at the LHC. The analysis is based on a data sample
             that was recorded in 2010 at a proton-proton center-of-mass
             energy of s=7 TeV and corresponds to an integrated
             luminosity of 34 pb-1. The cross section is measured in a
             region of high detector acceptance and then extrapolated to
             the full phase space. The product of the total W production
             cross section and the W→τντ branching ratio is measured
             to be σW→τντtot=11.1±0.3(stat)±1.7(syst)±0.4(lumi)
             nb. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.11.057},
   Key = {fds307751}
}

@article{fds356538,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
             Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V},
   Title = {Measurement of the Z(→ ℓ +)γ production cross-section in pp collisions at
             √s = 13 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {3},
   Year = {2020},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2020)054},
   Abstract = {The production of a prompt photon in association with a Z
             boson is studied in proton-proton collisions at a
             centre-of-mass energy s = 13 TeV. The analysis uses a data
             sample with an integrated luminosity of 139 fb−1 collected
             by the ATLAS detector at the LHC from 2015 to 2018. The
             production cross-section for the process pp → ℓ+ℓ−γ
             + X (ℓ = e, μ) is measured within a fiducial phase-space
             region defined by kinematic requirements on the photon and
             the leptons, and by isolation requirements on the photon. An
             experimental precision of 2.9% is achieved for the fiducial
             cross-section. Differential cross-sections are measured as a
             function of each of six kinematic variables characterising
             the ℓ+ℓ−γ system. The data are compared with
             theoretical predictions based on next-to-leading-order and
             next-to-next-to-leading-order perturbative QCD calculations.
             The impact of next-to-leading-order electroweak corrections
             is also considered. [Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP03(2020)054},
   Key = {fds356538}
}

@article{fds317301,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the Z/γ* boson transverse
             momentum distribution in pp collisions at √s = 7 TeV with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2014)145},
   Abstract = {This paper describes a measurement of the Z/γ* boson
             transverse momentum spectrum using ATLAS proton-proton
             collision data at a centre-of-mass energy of (Formula
             presented) TeV at the LHC. The measurement is performed in
             the Z/γ* → e+e− and Z/γ* → μ+μ− channels, using
             data corresponding to an integrated luminosity of 4.7
             fb−1. Normalized differential cross sections as a function
             of the Z/γ* boson transverse momentum are measured for
             transverse momenta up to 800 GeV. The measurement is
             performed inclusively for Z/γ* rapidities up to 2.4, as
             well as in three rapidity bins. The channel results are
             combined, compared to perturbative and resummed QCD
             calculations and used to constrain the parton shower
             parameters of Monte Carlo generators.},
   Doi = {10.1007/JHEP09(2014)145},
   Key = {fds317301}
}

@article{fds307714,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten,
             K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benjamin,
             DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius,
             C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan,
             JG and Coggeshall, J and Cogneras, E and Cojocaru,
             CD},
   Title = {Measurement of the ZZ production cross section and limits on
             anomalous neutral triple gauge couplings in proton-proton
             collisions at sqrt[s] = 7 TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {4},
   Pages = {041804},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.108.041804},
   Abstract = {A measurement of the ZZ production cross section in
             proton-proton collisions at sqrt[s] = 7 TeV using data
             corresponding to an integrated luminosity of 1.02 fb(-1)
             recorded by the ATLAS experiment at the LHC is presented.
             Twelve events containing two Z boson candidates decaying to
             electrons and/or muons are observed, with an expected
             background of 0.3 ± 0.3(stat)(-0.3)(+0.4)(syst) events. The
             cross section measured in a phase-space region with good
             detector acceptance and for dilepton masses within the range
             66 to 116 GeV is σ(ZZ → ℓ+ ℓ- ℓ+ ℓ-)(fid) =
             19.4(-5.2)(+6.3)(stat)(-0.7)(+0.9)(syst) ± 0.7(lumi) fb.
             The resulting total cross section for on-shell ZZ
             production, σ(ZZ)(tot) = 8.5(-2.3)(+2.7)(stat)(-0.3)(+0.4)(syst)
             ± 0.3(lumi) pb, is consistent with the standard model
             expectation of 6.5(-0.2)(+0.3) pb calculated at the
             next-to-leading order in QCD. Limits on anomalous neutral
             triple gauge boson couplings are derived.},
   Doi = {10.1103/physrevlett.108.041804},
   Key = {fds307714}
}

@article{fds347513,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
             Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
             C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram,
             IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia
             Bylund, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
             J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
             MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister,
             I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
             JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet,
             D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa,
             A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chouridou,
             S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou,
             Y},
   Title = {Measurement of the ZZ Production Cross Section in pp
             Collisions at sqrt[s]=13  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {116},
   Number = {10},
   Pages = {101801},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.116.101801},
   Abstract = {The ZZ production cross section in proton-proton collisions
             at 13 TeV center-of-mass energy is measured using
             3.2  fb^{-1} of data recorded with the ATLAS detector at
             the Large Hadron Collider. The considered Z boson candidates
             decay to an electron or muon pair of mass 66-116 GeV. The
             cross section is measured in a fiducial phase space
             reflecting the detector acceptance. It is also extrapolated
             to a total phase space for Z bosons in the same mass range
             and of all decay modes, giving 16.7_{-2.0}^{+2.2}(stat)+0.9/-0.7(syst)+1.0/-0.7(lumi)  pb.
             The results agree with standard model predictions.},
   Doi = {10.1103/physrevlett.116.101801},
   Key = {fds347513}
}

@article{fds356766,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Measurement of the ZZ production cross section in
             proton-proton collisions at √s=8 TeV using the ZZ →
             ℓ+′−′+
             and ZZ→ ℓ+νν¯ decay
             channels with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {1},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2017)099},
   Abstract = {A measurement of the ZZ production cross section in the
             ℓ−ℓ+ℓ′ −ℓ′ + and ℓ−ℓ+νν¯ channels
             (ℓ = e, μ) in proton-proton collisions at s=8TeV at the
             Large Hadron Collider at CERN, using data corresponding to
             an integrated luminosity of 20.3 fb−1 collected by the
             ATLAS experiment in 2012 is presented. The fiducial cross
             sections for ZZ → ℓ−ℓ+ℓ′ −ℓ′ + and ZZ→
             ℓ−ℓ+νν¯ are measured in selected phase-space
             regions. The total cross section for ZZ events produced with
             both Z bosons in the mass range 66 to 116 GeV is measured
             from the combination of the two channels to be 7.3 ±
             0.4(stat) ± 0.3(syst)− 0.1− 0.2(lumi) pb, which is
             consistent with the Standard Model prediction of 6. 6−
             0.6+ 0.7 pb. The differential cross sections in bins of
             various kinematic variables are presented. The differential
             event yield as a function of the transverse momentum of the
             leading Z boson is used to set limits on anomalous neutral
             triple gauge boson couplings in ZZ production.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP01(2017)099},
   Key = {fds356766}
}

@article{fds310379,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Measurement of the ZZ production cross section using the
             full CDF II data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.112001},
   Abstract = {We present a measurement of the ZZ-boson pair-production
             cross section in 1.96 TeV center-of-mass energy pp̄
             collisions. We reconstruct final states incorporating four
             charged leptons or two charged leptons and two neutrinos
             from the full data set collected by the Collider Detector
             experiment at the Fermilab Tevatron, corresponding to
             9.7fb-1 of integrated luminosity. Combining the results
             obtained from each final state, we measure a cross section
             of 1.04-0.25+0.32pb, in good agreement with the standard
             model prediction at next-to-leading order in the
             strong-interaction coupling. © 2014 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.89.112001},
   Key = {fds310379}
}

@article{fds347453,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {Measurement of the Zγ→ νν¯ γ production cross section
             in pp collisions at √s=13 TeV with the ATLAS detector and
             limits on anomalous triple gauge-boson couplings},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {12},
   Year = {2018},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2018)010},
   Abstract = {The production of Z bosons in association with a high-energy
             photon (Zγ production) is studied in the neutrino decay
             channel of the Z boson using pp collisions at s=13 TeV. The
             analysis uses a data sample with an integrated luminosity of
             36.1fb−1 collected by the ATLAS detector at the LHC in
             2015 and 2016. Candidate Zγ events with invisible decays of
             the Z boson are selected by requiring significant transverse
             momentum (pT) of the dineutrino system in conjunction with a
             single isolated photon with large transverse energy (ET).
             The rate of Zγ production is measured as a function of
             photon ET, dineutrino system pT and jet multiplicity.
             Evidence of anomalous triple gauge-boson couplings is sought
             in Zγ production with photon ET greater than 600 GeV. No
             excess is observed relative to the Standard Model
             expectation, and upper limits are set on the strength of
             ZZγ and Zγγ couplings.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP12(2018)010},
   Key = {fds347453}
}

@article{fds307854,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Measurement of the Z→ττ cross section with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {84},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.112006},
   Abstract = {The Z→ττ cross section is measured with the ATLAS
             experiment at the LHC in four different final states
             determined by the decay modes of the τ leptons:
             muon-hadron, electron-hadron, electron-muon, and muon-muon.
             The analysis is based on a data sample corresponding to an
             integrated luminosity of 36pb-1, at a proton-proton
             center-of-mass energy of √s=7TeV. Cross sections are
             measured separately for each final state in fiducial regions
             of high detector acceptance, as well as in the full phase
             space, over the mass region 66-116 GeV. The individual cross
             sections are combined and the product of the total Z
             production cross section and Z→ττ branching fraction is
             measured to be 0.97±0.07(stat)±0.06(syst)±0.03(lumi)nb,
             in agreement with next-to-next-to-leading order
             calculations. © 2011 CERN.},
   Doi = {10.1103/PhysRevD.84.112006},
   Key = {fds307854}
}

@article{fds347489,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett,
             RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr,
             AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
             M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone,
             RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli,
             A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
             Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont,
             AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark,
             MR},
   Title = {Measurement of the [Formula: see text] and [Formula: see
             text] production cross sections in multilepton final states
             using 3.2 fb[Formula: see text] of [Formula: see text]
             collisions at [Formula: see text] = 13 TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {1},
   Pages = {40},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4574-y},
   Abstract = {A measurement of the [Formula: see text] and [Formula: see
             text] production cross sections in final states with either
             two same-charge muons, or three or four leptons (electrons
             or muons) is presented. The analysis uses a data sample of
             proton-proton collisions at [Formula: see text] TeV recorded
             with the ATLAS detector at the Large Hadron Collider in
             2015, corresponding to a total integrated luminosity of
             3.2 fb[Formula: see text]. The inclusive cross sections are
             extracted using likelihood fits to signal and control
             regions, resulting in [Formula: see text] pb and [Formula:
             see text] pb, in agreement with the Standard Model
             predictions.},
   Doi = {10.1140/epjc/s10052-016-4574-y},
   Key = {fds347489}
}

@article{fds322001,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
             N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
             F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
             EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
             R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo,
             F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez,
             VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Measurement of the [Formula: see text] dijet cross section
             in pp collisions at [Formula: see text] TeV with the ATLAS
             detector.},
   Journal = {Eur Phys J C Part Fields},
   Volume = {76},
   Number = {12},
   Pages = {670},
   Year = {2016},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4521-y},
   Abstract = {The dijet production cross section for jets containing a
             b-hadron (b-jets) has been measured in proton-proton
             collisions with a centre-of-mass energy of [Formula: see
             text] TeV, using the ATLAS detector at the LHC. The data
             used correspond to an integrated luminosity of [Formula: see
             text]. The cross section is measured for events with two
             identified b-jets with a transverse momentum [Formula: see
             text] GeV and a minimum separation in the [Formula: see
             text]-[Formula: see text] plane of [Formula: see text]. At
             least one of the jets in the event is required to have
             [Formula: see text] GeV. The cross section is measured
             differentially as a function of dijet invariant mass, dijet
             transverse momentum, boost of the dijet system, and the
             rapidity difference, azimuthal angle and angular distance
             between the b-jets. The results are compared to different
             predictions of leading order and next-to-leading order
             perturbative quantum chromodynamics matrix elements
             supplemented with models for parton-showers and
             hadronization.},
   Doi = {10.1140/epjc/s10052-016-4521-y},
   Key = {fds322001}
}

@article{fds307616,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio,
             EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
             JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas,
             CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B},
   Title = {Measurement of the [Formula: see text] production cross
             section in the tau + jets channel using the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {3},
   Pages = {2328},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2328-7},
   Abstract = {A measurement of the top quark pair production cross section
             in the final state with a hadronically decaying tau lepton
             and jets is presented. The analysis is based on
             proton-proton collision data recorded by the ATLAS
             experiment at the LHC, with a centre-of-mass energy of
             7 TeV. The data sample corresponds to an integrated
             luminosity of 1.67 fb<sup>-1</sup>. The cross section is
             measured to be [Formula: see text] and is in agreement with
             other measurements and with the Standard Model
             prediction.},
   Doi = {10.1140/epjc/s10052-013-2328-7},
   Key = {fds307616}
}

@article{fds310393,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, MF and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
   Title = {Measurement of the [Formula: see text] production
             cross-section using [Formula: see text] events with
             [Formula: see text]-tagged jets in [Formula: see text]
             collisions at [Formula: see text] and 8 TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {10},
   Pages = {3109},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3109-7},
   Abstract = {The inclusive top quark pair ([Formula: see text])
             production cross-section [Formula: see text] has been
             measured in proton-proton collisions at [Formula: see text]
             and [Formula: see text] with the ATLAS experiment at the
             LHC, using [Formula: see text] events with an
             opposite-charge [Formula: see text] pair in the final state.
             The measurement was performed with the 2011 7 TeV dataset
             corresponding to an integrated luminosity of 4.6 [Formula:
             see text] and the 2012 8 TeV dataset of 20.3 [Formula: see
             text]. The numbers of events with exactly one and exactly
             two [Formula: see text]-tagged jets were counted and used to
             simultaneously determine [Formula: see text] and the
             efficiency to reconstruct and [Formula: see text]-tag a jet
             from a top quark decay, thereby minimising the associated
             systematic uncertainties. The cross-section was measured to
             be: [Formula: see text]where the four uncertainties arise
             from data statistics, experimental and theoretical
             systematic effects, knowledge of the integrated luminosity
             and of the LHC beam energy. The results are consistent with
             recent theoretical QCD calculations at next-to-next-to-leading
             order. Fiducial measurements corresponding to the
             experimental acceptance of the leptons are also reported,
             together with the ratio of cross-sections measured at the
             two centre-of-mass energies. The inclusive cross-section
             results were used to determine the top quark pole mass via
             the dependence of the theoretically predicted cross-section
             on [Formula: see text] giving a result of [Formula: see
             text][Formula: see text] GeV. By looking for an excess of
             [Formula: see text] production with respect to the QCD
             prediction, the results were also used to place limits on
             the pair-production of supersymmetric top squarks [Formula:
             see text] with masses close to the top quark mass, decaying
             via [Formula: see text] to predominantly right-handed top
             quarks and a light neutralino [Formula: see text], the
             lightest supersymmetric particle. Top squarks with masses
             between the top quark mass and 177 GeV are excluded at the
             95 % confidence level.},
   Doi = {10.1140/epjc/s10052-014-3109-7},
   Key = {fds310393}
}

@article{fds307629,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Measurement of the Λb0 lifetime and mass in the ATLAS
             experiment},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.032002},
   Abstract = {A measurement of the Λb0 lifetime and mass in the decay
             channel Λb0→J/ψ(μ+μ-)Λ0(pπ -) is presented. The
             analysis uses a signal sample of about 2200 Λb0 and Λ̄b0
             decays that are reconstructed in 4.9 fb -1 of ATLAS pp
             collision data collected in 2011 at the LHC center-of-mass
             energy of 7 TeV. A simultaneous mass and decay time maximum
             likelihood fit is used to extract the Λb0 lifetime and
             mass. They are measured to be τΛb=1.449±0.036(stat)
             ±0.017(syst) ps and mΛb=5619.7±0. 7(stat)±1.1(syst)
             MeV.},
   Doi = {10.1103/PhysRevD.87.032002},
   Key = {fds307629}
}

@article{fds344670,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carrillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
             M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully,
             JC and Cyr, D and Daronco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng,
             J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and Dituro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube,
             S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
             I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Gimmell, JL and Ginsburg,
             C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute,
             M and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Labarga, L and Lai, S and Lami, S and Lammel,
             S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
             C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
             D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
             P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino,
             C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
             M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt,
             J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman,
             J and Nagano, A and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prokoshin, F and Pronko, A and Proudfoot, J and Ptochos, F and Punzi, G and Pursley, J and Rademacker,
             J and Rahaman, A and Ranjan, N and Rappoccio, S and Reisert, B and Rekovic,
             V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
             L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti,
             A},
   Title = {Measurement of the Λb0 Lifetime in Λb0→J/ψΛ0 in pp̄
             Collisions at s=1.96TeV},
   Journal = {Physical Review Letters},
   Volume = {98},
   Number = {12},
   Pages = {122001},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.98.122001},
   Abstract = {We report a measurement of the Λb0 lifetime in the
             exclusive decay Λb0→J/ψΛ0 in pp̄ collisions at
             s=1.96TeV using an integrated luminosity of 1.0fb-1 of data
             collected by the CDF II detector at the Fermilab Tevatron.
             Using fully reconstructed decays, we measure
             τ(Λb0)=1.593-0.078+0.083(stat)±0.033(syst)ps. This is the
             single most precise measurement of τ(Λb0) and is 3.2σ
             higher than the current world average. © 2007 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.98.122001},
   Key = {fds344670}
}

@article{fds307864,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R and Ask, S},
   Title = {Measurement of the Υ(1S) production cross-section in pp
             collisions at s=7 TeV in ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {1-2},
   Pages = {9-27},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.09.092},
   Abstract = {A measurement of the cross-section for Υ(1S)→μ+μ-
             production in proton-proton collisions at centre of mass
             energy of 7 TeV is presented. The cross-section is measured
             as a function of the Υ(1S) transverse momentum in two bins
             of rapidity, |yΥ(1S)|<1.2 and 1.2<|yΥ(1S)|<2.4. The
             measurement requires that both muons have transverse
             momentum pTμ>4 GeV and pseudorapidity |ημ|<2.5 in order
             to reduce theoretical uncertainties on the acceptance, which
             depend on the poorly known polarisation. The results are
             based on an integrated luminosity of 1.13 pb-1, collected
             with the ATLAS detector at the Large Hadron Collider. The
             cross-section measurement is compared to theoretical
             predictions: it agrees to within a factor of two with a
             prediction based on the NRQCD model including colour-singlet
             and colour-octet matrix elements as implemented in Pythia
             while it disagrees by up to a factor of ten with the
             next-to-leading order prediction based on the colour-singlet
             model. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.09.092},
   Key = {fds307864}
}

@article{fds310322,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
   Title = {Measurement of three-jet production cross-sections in
             [Formula: see text] collisions at 7 [Formula: see text]
             centre-of-mass energy using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {5},
   Pages = {228},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3363-3},
   Abstract = {Double-differential three-jet production cross-sections are
             measured in proton-proton collisions at a centre-of-mass
             energy of [Formula: see text] using the ATLAS detector at
             the large hadron collider. The measurements are presented as
             a function of the three-jet mass [Formula: see text], in
             bins of the sum of the absolute rapidity separations between
             the three leading jets [Formula: see text]. Invariant masses
             extending up to 5  TeV are reached for [Formula: see
             text]. These measurements use a sample of data recorded
             using the ATLAS detector in 2011, which corresponds to an
             integrated luminosity of [Formula: see text]. Jets are
             identified using the anti-[Formula: see text] algorithm with
             two different jet radius parameters, [Formula: see text] and
             [Formula: see text]. The dominant uncertainty in these
             measurements comes from the jet energy scale.
             Next-to-leading-order QCD calculations corrected to account
             for non-perturbative effects are compared to the
             measurements. Good agreement is found between the data and
             the theoretical predictions based on most of the available
             sets of parton distribution functions, over the full
             kinematic range, covering almost seven orders of magnitude
             in the measured cross-section values.},
   Doi = {10.1140/epjc/s10052-015-3363-3},
   Key = {fds310322}
}

@article{fds321077,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of top quark pair differential cross sections in
             the dilepton channel in pp collisions at √s =7 and 8 TeV
             with ATLAS},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.092003},
   Abstract = {Measurements of normalized differential cross sections of
             top quark pair (tt production are presented as a function of
             the mass, the transverse momentum and the rapidity of the tt
             system in proton-proton collisions at center-of-mass
             energies of s=7 and 8 TeV. The data set corresponds to an
             integrated luminosity of 4.6 fb-1 at 7 TeV and 20.2 fb-1 at
             8 TeV, recorded with the ATLAS detector at the Large Hadron
             Collider. Events with top quark pair signatures are selected
             in the dilepton final state, requiring exactly two charged
             leptons and at least two jets with at least one of the jets
             identified as likely to contain a b hadron. The measured
             distributions are corrected for detector effects and
             selection efficiency to cross sections at the parton level.
             The differential cross sections are compared with different
             Monte Carlo generators and theoretical calculations of tt
             production. The results are consistent with the majority of
             predictions in a wide kinematic range.},
   Doi = {10.1103/PhysRevD.94.092003},
   Key = {fds321077}
}

@article{fds307557,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov,
             A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith,
             L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay,
             NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
             G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach,
             AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
             P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernhard, R and Bernius, C and Bernlochner,
             FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Buehrer, F and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ},
   Title = {Measurement of top quark polarization in top-antitop events
             from proton-proton collisions at √s=7  TeV using the
             ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {23},
   Pages = {232002},
   Year = {2013},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.111.232002},
   Abstract = {This Letter presents measurements of the polarization of the
             top quark in top-antitop quark pair events, using
             4.7  fb(-1) of proton-proton collision data recorded
             with the ATLAS detector at the Large Hadron Collider at
             √s=7  TeV. Final states containing one or two isolated
             leptons (electrons or muons) and jets are considered. Two
             measurements of α(ℓ)P, the product of the leptonic
             spin-analyzing power and the top quark polarization, are
             performed assuming that the polarization is introduced by
             either a CP conserving or a maximally CP violating
             production process. The measurements obtained,
             α(ℓ)P(CPC)=-0.035±0.014(stat)±0.037(syst) and
             α(ℓ)P(CPV)=0.020±0.016(stat)(-0.017)(+0.013)(syst), are
             in good agreement with the standard model prediction of
             negligible top quark polarization.},
   Doi = {10.1103/physrevlett.111.232002},
   Key = {fds307557}
}

@article{fds321092,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Measurement of total and differential W + W
              production cross sections in proton-proton
             collisions at √s=8 TeV with the ATLAS detector and limits
             on anomalous triple-gauge-boson couplings},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2016)029},
   Abstract = {The production of W boson pairs in proton-proton collisions
             at s=8 TeV is studied using data corresponding to 20.3
             fb−1 of integrated luminosity collected by the ATLAS
             detector during 2012 at the CERN Large Hadron Collider. The
             W bosons are reconstructed using their leptonic decays into
             electrons or muons and neutrinos. Events with reconstructed
             jets are not included in the candidate event sample. A total
             of 6636 WW candidate events are observed. Measurements are
             performed in fiducial regions closely approximating the
             detector acceptance. The integrated measurement is corrected
             for all acceptance effects and for the W branching fractions
             to leptons in order to obtain the total WW production cross
             section, which is found to be 71.1 ± 1.1(stat) − 5.0+
             5.7(syst) ± 1.4(lumi) pb. This agrees with the
             next-to-next-to-leading-order Standard Model prediction of
             63. 2− 1.4+ 1.6(scale) ± 1.2(PDF) pb. Fiducial
             differential cross sections are measured as a function of
             each of six kinematic variables. The distribution of the
             transverse momentum of the leading lepton is used to set
             limits on anomalous triple-gauge-boson couplings.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP09(2016)029},
   Key = {fds321092}
}

@article{fds321135,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åesson, TPA and Akimov, AV and Alberghi,
             GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and varez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of transverse energy-energy correlations in
             multi-jet events in pp collisions at s=7 TeV using the ATLAS
             detector and determination of the strong coupling constant
             as(mZ)},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {750},
   Pages = {427-447},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.09.050},
   Abstract = {High transverse momentum jets produced in pp collisions at a
             centre of mass energy of 7 TeV are used to measure the
             transverse energy-energy correlation function and its
             associated azimuthal asymmetry. The data were recorded with
             the ATLAS detector at the LHC in the year 2011 and
             correspond to an integrated luminosity of 158 pb-1. The
             selection criteria demand the average transverse momentum of
             the two leading jets in an event to be larger than 250 GeV.
             The data at detector level are well described by Monte Carlo
             event generators. They are unfolded to the particle level
             and compared with theoretical calculations at
             next-to-leading-order accuracy. The agreement between data
             and theory is good and provides a precision test of
             perturbative Quantum Chromodynamics at large momentum
             transfers. From this comparison, the strong coupling
             constant given at the Z boson mass is determined to be
             as(mZ)=0.1173±0.0010 (exp.) -0.0026+0.0065
             (theo.).},
   Doi = {10.1016/j.physletb.2015.09.050},
   Key = {fds321135}
}

@article{fds307614,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Measurement of upsilon production in 7 TeV pp collisions at
             ATLAS},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.052004},
   Abstract = {Using 1.8 fb-1 of pp collisions at a center-of-mass energy
             of 7 TeV recorded by the ATLAS detector at the Large Hadron
             Collider, we present measurements of the production cross
             sections of Υ(1S,2S,3S) mesons. Υ mesons are reconstructed
             using the dimuon decay mode. Total production cross sections
             for pT<70 GeV and in the rapidity interval |yΥ|<2.25 are
             measured to be, 8.01±0.02±0.36±0.31 nb,
             2.05±0.01±0.12±0.08 nb, and 0.92±0.01±0. 07±0.04 nb,
             respectively, with uncertainties separated into statistical,
             systematic, and luminosity measurement effects. In addition,
             differential cross section times dimuon branching fractions
             for Υ(1S), Υ(2S), and Υ(3S) as a function of Υ
             transverse momentum pT and rapidity are presented. These
             cross sections are obtained assuming unpolarized production.
             If the production polarization is fully transverse or
             longitudinal with no azimuthal dependence in the helicity
             frame, the cross section may vary by approximately ±20%. If
             a nontrivial azimuthal dependence is considered, integrated
             cross sections may be significantly enhanced by a factor of
             2 or more. We compare our results to several theoretical
             models of Υ meson production, finding that none provide an
             accurate description of our data over the full range of Υ
             transverse momenta accessible with this data
             set.},
   Doi = {10.1103/PhysRevD.87.052004},
   Key = {fds307614}
}

@article{fds314800,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Measurement of vector boson plus D∗ (2010)+ meson
             production in p-p collisions at s =1.96 TeV MEASUREMENT of
             VECTOR BOSON PLUS D∗ (2010)+ ... T. AALTONEN et
             al.},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {March},
   ISSN = {2470-0010},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.052012},
   Abstract = {A measurement of vector boson (V) production in conjunction
             with a D∗(2010)+ meson is presented. Using a data sample
             corresponding to 9.7 fb-1 of proton-antiproton collisions at
             center-of-mass energy s=1.96 TeV produced by the Fermilab
             Tevatron, we reconstruct V+D∗+ samples with the CDF II
             detector. The D∗+ is fully reconstructed in the
             D∗(2010)+→D0(→K-π+)π+ decay mode. This technique is
             sensitive to the associated production of vector boson plus
             charm or bottom mesons. We measure the ratio of production
             cross sections σ(W+D∗)/σ(W)=[1.75±0.13(stat)±0.09(stat)]%
             and σ(Z+D∗)/σ(Z)=[1.5±0.4(stat)±0.2(stat)]% and
             perform a differential measurement of dσ(W+D∗)/dpT(D∗).
             Event properties are utilized to determine the fraction of
             V+D∗(2010)+ events originating from different production
             processes. The results are in agreement with the predictions
             obtained with the pythia program, limiting possible
             contribution from non-standard-model physics
             processes.},
   Doi = {10.1103/PhysRevD.93.052012},
   Key = {fds314800}
}

@article{fds356604,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
             Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
             NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli,
             E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V},
   Title = {Measurement of VH, H → b b ¯ production as a function of
             the vector-boson transverse momentum in 13 TeV pp collisions
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {5},
   Year = {2019},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2019)141},
   Abstract = {Cross-sections of associated production of a Higgs boson
             decaying into bottomquark pairs and an electroweak gauge
             boson, W or Z, decaying into leptons are measured as a
             function of the gauge boson transverse momentum. The
             measurements are performed in kinematic fiducial volumes
             defined in the ‘simplified template cross-section’
             framework. The results are obtained using 79.8 fb−1 of
             proton-proton collisions recorded by the ATLAS detector at
             the Large Hadron Collider at a centre-of-mass energy of 13
             TeV. All measurements are found to be in agreement with the
             Standard Model predictions, and limits are set on the
             parameters of an effective Lagrangian sensitive to
             modifications of the Higgs boson couplings to the
             electroweak gauge bosons.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP05(2019)141},
   Key = {fds356604}
}

@article{fds308225,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Alves, GA and Amos, N and Anderson,
             EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov,
             VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
             K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
             SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
             Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison,
             J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher,
             S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE and Fortner, M and Frame, KC},
   Title = {Measurement of W and Z boson production cross sections in
             [formula presented] collisions at [formula presented]
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {60},
   Number = {5},
   Pages = {1-21},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.60.052003},
   Abstract = {DØhas measured the inclusive production cross section of W
             and Z bosons in a sample of 13 (Formula presented) of data
             collected at the Fermilab Tevatron. The cross sections,
             multiplied by their leptonic branching fractions, for
             production in (Formula presented) collisions at (Formula
             presented) TeV are (Formula presented) (Formula presented)
             (Formula presented), and (Formula presented), where the
             first uncertainty is statistical and the second systematic;
             the third reflects the uncertainty in the integrated
             luminosity. For the combined electron and muon analyses, we
             find (Formula presented). Assuming standard model couplings,
             we use this result to determine the width of the W boson,
             and obtain (Formula presented). © 1999 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.60.052003},
   Key = {fds308225}
}

@article{fds356761,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of W boson angular distributions in events with
             high transverse momentum jets at √s=8 TeV using the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {765},
   Pages = {132-153},
   Year = {2017},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.12.005},
   Abstract = {The W boson angular distribution in events with high
             transverse momentum jets is measured using data collected by
             the ATLAS experiment from proton–proton collisions at a
             centre-of-mass energy s=8 TeV at the Large Hadron Collider,
             corresponding to an integrated luminosity of 20.3 fb−1.
             The focus is on the contributions to W+jets processes from
             real W emission, which is achieved by studying events where
             a muon is observed close to a high transverse momentum jet.
             At small angular separations, these contributions are
             expected to be large. Various theoretical models of this
             process are compared to the data in terms of the absolute
             cross-section and the angular distributions of the muon from
             the leptonic W decay.},
   Doi = {10.1016/j.physletb.2016.12.005},
   Key = {fds356761}
}

@article{fds348982,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines,
             JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann,
             TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
             NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
             TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro,
             R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn,
             R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
             JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark,
             MR},
   Title = {Measurement of W W / W Z → ℓ ν q q ' production with
             the hadronically decaying boson reconstructed as one or two
             jets in pp collisions at s = 8 TeV with ATLAS, and
             constraints on anomalous gauge couplings.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {8},
   Pages = {563},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5084-2},
   Abstract = {This paper presents a study of the production of <i>WW</i>
             or <i>WZ</i> boson pairs, with one <i>W</i> boson decaying
             to e ν or μ ν and one <i>W</i> or <i>Z</i> boson decaying
             hadronically. The analysis uses 20.2 fb - 1 of s = 8 TeV
             <i>pp</i> collision data, collected by the ATLAS detector at
             the Large Hadron Collider. Cross-sections for
             <i>WW</i> / <i>WZ</i> production are measured in high- p T
             fiducial regions defined close to the experimental event
             selection. The cross-section is measured for the case where
             the hadronically decaying boson is reconstructed as two
             resolved jets, and the case where it is reconstructed as a
             single jet. The transverse momentum distribution of the
             hadronically decaying boson is used to search for new
             physics. Observations are consistent with the Standard Model
             predictions, and 95% confidence intervals are calculated for
             parameters describing anomalous triple gauge-boson
             couplings.},
   Doi = {10.1140/epjc/s10052-017-5084-2},
   Key = {fds348982}
}

@article{fds307988,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D},
   Title = {Measurement of W-boson helicity fractions in top-quark
             decays using cos θ*},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {674},
   Number = {3},
   Pages = {160-167},
   Publisher = {Elsevier BV},
   Year = {2009},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2009.02.040},
   Abstract = {Fully reconstructed t over(t, ̄) → W+ b W- over(b, ̄)
             → ℓ ν q over(q, ̄)′ b over(b, ̄) events are used to
             determine the fractions of right-handed (f+) and
             longitudinally polarized (f0) W bosons produced in top-quark
             decays. The helicity fractions are sensitive to the
             couplings and the Dirac structure of the Wtb vertex. This
             Letter reports measurements of the W-boson helicity
             fractions from two different methods using data
             corresponding to an integrated luminosity of 1.9 fb- 1 of p
             over(p, ̄) collisions at a center-of-mass energy of 1.96
             TeV collected by the CDF II detector operating at the
             Fermilab Tevatron. Combining the results from the two
             methods, we find f0 = 0.62 ± 0.10 (stat) ± 0.05 (syst)
             under the assumption that f+ = 0, and f+ = - 0.04 ± 0.04
             (stat) ± 0.03 (syst) with f0 fixed to the theoretically
             expected value of 0.70. Model-independent fits are also
             performed and simultaneously determine f0 = 0.66 ± 0.16
             (stat) ± 0.05 (syst) and f+ = - 0.03 ± 0.06 (stat) ± 0.03
             (syst). All these results are consistent with standard model
             expectations. © 2009 Elsevier B.V.},
   Doi = {10.1016/j.physletb.2009.02.040},
   Key = {fds307988}
}

@article{fds307900,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of W-Boson Polarization in Top-Quark Decay in
             ppbar Collisions at sqrt{s}=1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {4},
   Pages = {042002},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.042002},
   Abstract = {We report measurements of the polarization of W bosons from
             top-quark decays using 2.7 fb{-1} of pp collisions collected
             by the CDF II detector. Assuming a top-quark mass of
             175  GeV/c{2}, three measurements are performed. A
             simultaneous measurement of the fraction of longitudinal
             (f{0}) and right-handed (f{+}) W bosons yields the
             model-independent results f{0}=0.88±0.11(stat)±0.06(syst)
             and f{+}=-0.15±0.07(stat)±0.06(syst) with a correlation
             coefficient of -0.59. A measurement of f{0} [f{+}]
             constraining f{+} [f{0}] to its standard model value of 0.0
             [0.7] yields f{0}=0.70±0.07(stat)±0.04(syst)
             [f{+}=-0.01±0.02(stat)±0.05(syst)]. All these results are
             consistent with standard model expectations. We achieve the
             single most precise measurements of f{0} for both the
             model-independent and model-dependent determinations.},
   Doi = {10.1103/PhysRevLett.105.042002},
   Key = {fds307900}
}

@article{fds307627,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Measurement of W-boson polarization in top-quark decay using
             the full CDF Run II data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.031104},
   Abstract = {We measure the polarization of W bosons from top-quark (t)
             decays into final states with a charged lepton and jets,
             tt̄→W+bW -b̄→ℓνbqq̄′b̄, using the full Run II
             data set collected by the CDF II detector, corresponding to
             an integrated luminosity of 8.7 fb-1. A model-independent
             method simultaneously determines the fraction of
             longitudinal (f0) and right-handed (f+) W bosons to yield
             f0=0.726±0. 066(stat)±0.067(syst) and f+=-0.045±0.044(stat)
             ±0.058(syst) with a correlation coefficient of -0.69.
             Additional results are presented under various standard
             model assumptions. No significant discrepancies with the
             standard model are observed. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.87.031104},
   Key = {fds307627}
}

@article{fds313632,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery,
             M},
   Title = {Measurement of Wγ and Zγ production
             in pp̄ collisions at √s = 1.96 TeV},
   Journal = {Physical Review Letters},
   Volume = {94},
   Number = {4},
   Year = {2005},
   Month = {February},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.94.041803},
   Abstract = {The standard model predictions for Wγ and Z γ production
             are tested using an integrated luminosity of 200 pb-1 of
             pp̄ collision data collected at the Collider Detector at
             Fermilab. The cross sections are measured by selecting
             leptonic decays of the W and Z bosons, and photons with
             transverse energy ET > 7 GeV that are well separated from
             leptons. The production cross sections and kinematic
             distributions for the Wγ and Zγ data are compared to SM
             predictions. © 2005 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.94.041803},
   Key = {fds313632}
}

@article{fds307598,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, JF and Arik, E},
   Title = {Measurement of W+W- production in pp
             collisions at √s=7 TeV with the ATLAS detector and limits
             on anomalous WWZ and WWγ couplings},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.112001},
   Abstract = {This paper presents a measurement of the W+W- production
             cross section in pp collisions at √s=7 TeV. The leptonic
             decay channels are analyzed using data corresponding to an
             integrated luminosity of 4.6 fb-1 collected with the ATLAS
             detector at the Large Hadron Collider. The W+W- production
             cross section σ(pp→W+W-+X) is measured to be
             51.9±2.0(stat)±3.9(syst)±2.0(lumi) pb, compatible with
             the Standard Model prediction of 44.7-1.9+2.1 pb. A
             measurement of the normalized fiducial cross section as a
             function of the leading lepton transverse momentum is also
             presented. The reconstructed transverse momentum
             distribution of the leading lepton is used to extract limits
             on anomalous WWZ and WWγ couplings.},
   Doi = {10.1103/PhysRevD.87.112001},
   Key = {fds307598}
}

@article{fds322934,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and AlconadaVerzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of W+W-production in
             association with one jet in proton-proton collisions at √s
             = 8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {763},
   Pages = {114-133},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.10.014},
   Abstract = {The production of Wboson pairs in association with one jet
             in pp collisions at √s = 8 TeV is studied using data
             corresponding to an integrated luminosity of 20.3
             fb-1collected by the ATLAS detector during 2012 at the CERN
             Large Hadron Collider. The cross section is measured in a
             fiducial phase-space region defined by the presence of
             exactly one electron and one muon, missing transverse
             momentum and exactly one jet with a transverse momentum
             above 25 GeV and a pseudorapidity of |η| <4.5. The leptons
             are required to have opposite electric charge and to pass
             transverse momentum and pseudorapidity requirements. The
             fiducial cross section is found to be σWWfid,1-jet= 136 ±
             6 (stat)± 14 (syst)± 3 (lumi) fb. In combination with a
             previous measurement restricted to leptonic final states
             with no associated jets, the fiducial cross section of WW
             production with zero or one jet is measured to be
             σWWfid,≤1-jet= 511 ±9 (stat)±26 (syst)±10 (lumi)fb.
             The ratio of fiducial cross sections in final states with
             one and zero jets is determined to be 0.36 ±0.05. Finally,
             a total cross section extrapolated from the fiducial
             measurement of WW production with zero or one associated jet
             is reported. The measurements are compared to theoretical
             predictions and found in good agreement.},
   Doi = {10.1016/j.physletb.2016.10.014},
   Key = {fds322934}
}

@article{fds356562,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
             L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
             JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA},
   Title = {Measurement of W± -boson and Z-boson production
             cross-sections in pp collisions at √s=2.76 TeV with the
             ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {11},
   Year = {2019},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7399-7},
   Abstract = {The production cross-sections for W± and Z bosons are
             measured using ATLAS data corresponding to an integrated
             luminosity of 4.0 pb- 1 collected at a centre-of-mass
             energy s=2.76 TeV. The decay channels W→ ℓν and Z→
             ℓℓ are used, where ℓ can be an electron or a muon. The
             cross-sections are presented for a fiducial region defined
             by the detector acceptance and are also extrapolated to the
             full phase space for the total inclusive production
             cross-section. The combined (average) total inclusive
             cross-sections for the electron and muon channels are:
             σW+→ℓνtot=2312±26(stat.)±27(syst.)±72(lumi.)±30(extr.)pb,σW-→ℓνtot=1399±21(stat.)±17(syst.)±43(lumi.)±21(extr.)pb,σZ→ℓℓtot=323.4±9.8(stat.)±5.0(syst.)±10.0(lumi.)±5.5(extr.)pb.Measured
             ratios and asymmetries constructed using these
             cross-sections are also presented. These observables benefit
             from full or partial cancellation of many systematic
             uncertainties that are correlated between the different
             measurements.},
   Doi = {10.1140/epjc/s10052-019-7399-7},
   Key = {fds356562}
}

@article{fds321102,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Measurement of W± and Z-boson production cross
             sections in pp collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {759},
   Pages = {601-621},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.06.023},
   Abstract = {Measurements of the W±→ℓ±ν and Z→ℓ+ℓ−
             production cross sections (where ℓ±=e±,μ±) in
             proton–proton collisions at s=13 TeV are presented using
             data recorded by the ATLAS experiment at the Large Hadron
             Collider, corresponding to a total integrated luminosity of
             81 pb−1. The total inclusive W±-boson production cross
             sections times the single-lepton-flavour branching ratios
             are σW+tot=11.83±0.02 (stat)±0.32 (sys)±0.25 (lumi) nb
             and σW−tot=8.79±0.02 (stat)±0.24 (sys)±0.18 (lumi) nb
             for W+ and W−, respectively. The total inclusive Z-boson
             production cross section times leptonic branching ratio,
             within the invariant mass window 66<mℓℓ<116 GeV, is
             σZtot=1.981±0.007 (stat)±0.038 (sys)±0.042 (lumi) nb.
             The W+, W−, and Z-boson production cross sections and
             cross-section ratios within a fiducial region defined by the
             detector acceptance are also measured. The cross-section
             ratios benefit from significant cancellation of experimental
             uncertainties, resulting in σW+fid/σW−fid=1.295±0.003
             (stat)±0.010 (sys) and σW±fid/σZfid=10.31±0.04
             (stat)±0.20 (sys). Theoretical predictions, based on
             calculations accurate to next-to-next-to-leading order for
             quantum chromodynamics and to next-to-leading order for
             electroweak processes and which employ different parton
             distribution function sets, are compared to these
             measurements.},
   Doi = {10.1016/j.physletb.2016.06.023},
   Key = {fds321102}
}

@article{fds356563,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA and Pereira,
             RA},
   Title = {Measurement of W± boson production in Pb+Pb
             collisions at √sNN=5.02Te with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {11},
   Year = {2019},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7439-3},
   Abstract = {A measurement of W± boson production in Pb+Pb collisions at
             sNN=5.02Te is reported using data recorded by the ATLAS
             experiment at the LHC in 2015, corresponding to a total
             integrated luminosity of 0.49nb-1. The W± bosons are
             reconstructed in the electron or muon leptonic decay
             channels. Production yields of leptonically decaying W±
             bosons, normalised by the total number of minimum-bias
             events and the nuclear thickness function, are measured
             within a fiducial region defined by the detector acceptance
             and the main kinematic requirements. These normalised yields
             are measured separately for W+ and W- bosons, and are
             presented as a function of the absolute value of
             pseudorapidity of the charged lepton and of the collision
             centrality. The lepton charge asymmetry is also measured as
             a function of the absolute value of lepton pseudorapidity.
             In addition, nuclear modification factors are calculated
             using the W± boson production cross-sections measured in pp
             collisions. The results are compared with predictions based
             on next-to-leading-order calculations with CT14 parton
             distribution functions as well as with predictions obtained
             with the EPPS16 and nCTEQ15 nuclear parton distribution
             functions. No dependence of normalised production yields on
             centrality and a good agreement with predictions are
             observed for mid-central and central collisions. For
             peripheral collisions, the data agree with predictions
             within 1.7 (0.9) standard deviations for W- (W+)
             bosons.},
   Doi = {10.1140/epjc/s10052-019-7439-3},
   Key = {fds356563}
}

@article{fds356594,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster,
             AJ},
   Title = {Measurement of W±Z production cross sections and
             gauge boson polarisation in pp collisions at √s=13TeV with
             the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {6},
   Year = {2019},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7027-6},
   Abstract = {This paper presents measurements of W±Z production cross
             sections in pp collisions at a centre-of-mass energy of
             13 TeV. The data were collected in 2015 and 2016 by the
             ATLAS experiment at the Large Hadron Collider, and
             correspond to an integrated luminosity of 36.1fb-1. The W±Z
             candidate events are reconstructed using leptonic decay
             modes of the gauge bosons into electrons and muons. The
             measured inclusive cross section in the detector fiducial
             region for a single leptonic decay mode is
             σW±Z→ℓ′νℓℓfid.=63.7±1.0(stat.)±2.3(syst.)±1.4(lumi.) fb,
             reproduced by the next-to-next-to-leading-order Standard
             Model prediction of 61.5-1.3+1.4 fb. Cross sections for W+Z
             and W-Z production and their ratio are presented as well as
             differential cross sections for several kinematic
             observables. An analysis of angular distributions of leptons
             from decays of W and Z bosons is performed for the first
             time in pair-produced events in hadronic collisions, and
             integrated helicity fractions in the detector fiducial
             region are measured for the W and Z bosons separately. Of
             particular interest, the longitudinal helicity fraction of
             pair-produced vector bosons is also measured.},
   Doi = {10.1140/epjc/s10052-019-7027-6},
   Key = {fds356594}
}

@article{fds307683,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim, A and Amram,
             N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M},
   Title = {Measurement of W±Z production in proton-proton
             collisions At √s = 7 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2173-0},
   Abstract = {A study of W ± Z production in proton-proton collisions at
             √s = 7 TeV is presented using data corresponding to an
             integrated luminosity of 4.6 fb−1 collected with the ATLAS
             detector at the Large Hadron Collider in 2011. In total, 317
             candidates, with a background expectation of 68 ± 10
             events, are observed in double-leptonic decay final states
             with electrons, muons and missing transverse momentum. The
             total cross-section is determined to be be σtotWZ =
             19.0+1.4−1.3 (stat.) ± 0.9(syst.) ± 0.4(lumi.) pb,
             consistent with the Standard Model expectation of
             17.6+1.1−1.0 pb. Limits on anomalous triple gauge boson
             couplings are derived using the transverse momentum spectrum
             of Z bosons in the selected events. The cross-section is
             also presented as a function of Z boson transverse momentum
             and diboson invariant mass.},
   Doi = {10.1140/epjc/s10052-012-2173-0},
   Key = {fds307683}
}

@article{fds356768,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of W±W± vector-boson scattering and limits on
             anomalous quartic gauge couplings with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {96},
   Number = {1},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.96.012007},
   Abstract = {This paper presents the extended results of measurements of
             W±W±jj production and limits on anomalous quartic gauge
             couplings using 20.3 fb-1 of proton-proton collision data at
             s=8 TeV recorded by the ATLAS detector at the Large Hadron
             Collider. Events with two leptons (e or μ) with the same
             electric charge and at least two jets are analyzed.
             Production cross sections are determined in two fiducial
             regions, with different sensitivities to the electroweak and
             strong production mechanisms. An additional fiducial region,
             particularly sensitive to anomalous quartic gauge coupling
             parameters α4 and α5, is introduced, which allows more
             stringent limits on these parameters compared to the
             previous ATLAS measurement.},
   Doi = {10.1103/PhysRevD.96.012007},
   Key = {fds356768}
}

@article{fds307793,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D},
   Title = {Measurement of Wγ and Zγ production cross sections in pp
             collisions at √s=7 TeV and limits on anomalous triple
             gauge couplings with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {717},
   Number = {1-3},
   Pages = {49-69},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {October},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.09.017},
   Abstract = {This Letter presents measurements of l±νγ and l+l−γ
             (l=e,μ) production in 1.02 fb−1 of pp collision data
             recorded at s=7 TeV with the ATLAS detector at the LHC in
             the first half of 2011. Events dominated by Wγ and Zγ
             production with leptonic decays of the W and Z bosons are
             selected, and their production cross sections and kinematic
             properties are measured in several ranges of the photon
             transverse energy. The results are compared to Standard
             Model predictions and are used to determine limits on
             anomalous WWγ and ZZγ/Zγγ couplings.},
   Doi = {10.1016/j.physletb.2012.09.017},
   Key = {fds307793}
}

@article{fds325780,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai,
             S},
   Title = {Measurement of Wγ and Zγ production in proton-proton
             collisions at √s = 7 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2011},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP09(2011)072},
   Abstract = {We present studies of W and Z bosons with associated high
             energy photons produced in pp collisions at √s = 7TeV. The
             analysis uses 35 pb γ + X) event candidates are selected.
             The kinematic distributions of the leptons and photons and
             the production cross sections are measured. The data are
             found to agree with Standard Model predictions that include
             next-to-leading-order O(ααs) contributions. © SISSA
             2011.},
   Doi = {10.1007/JHEP09(2011)072},
   Key = {fds325780}
}

@article{fds307635,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
             R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez
             Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
             A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland,
             W},
   Title = {Measurement of Z boson production in Pb-Pb collisions at
             sqrt[s(NN)]=2.76  TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {2},
   Pages = {022301},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.110.022301},
   Abstract = {The ATLAS experiment has observed 1995 Z boson candidates in
             data corresponding to 0.15  nb(-1) of integrated
             luminosity obtained in the 2011 LHC Pb+Pb run at
             sqrt[s(NN)]=2.76  TeV. The Z bosons are reconstructed
             via dielectron and dimuon decay channels, with a background
             contamination of less than 3%. Results from the two channels
             are consistent and are combined. Within the statistical and
             systematic uncertainties, the per-event Z boson yield is
             proportional to the number of binary collisions estimated by
             the Glauber model. The elliptic anisotropy of the azimuthal
             distribution of the Z boson with respect to the event plane
             is found to be consistent with zero.},
   Doi = {10.1103/physrevlett.110.022301},
   Key = {fds307635}
}

@article{fds307712,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of ZZ production in leptonic final states at
             sqrt[s] of 1.96 TeV at CDF.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {10},
   Pages = {101801},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.108.101801},
   Abstract = {In this Letter, we present a precise measurement of the
             total ZZ production cross section in pp collisions at
             sqrt[s]=1.96  TeV, using data collected with the CDF II
             detector corresponding to an integrated luminosity of
             approximately 6  fb(-1). The result is obtained by
             combining separate measurements in the four-charged
             (ℓℓℓ' ℓ') and two-charged-lepton and
             two-neutral-lepton (ℓℓνν) decay modes of the Z boson
             pair. The combined measured cross section for pp → ZZ is
             1.64(-0.38)(+0.44)  pb. This is the most precise
             measurement of the ZZ production cross section in 1.96 TeV
             pp collisions to date.},
   Doi = {10.1103/physrevlett.108.101801},
   Key = {fds307712}
}

@article{fds307618,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Measurement of ZZ production in pp collisions at √ = 7 TeV
             and limits on anomalous ZZZ and ZZγ couplings with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2013)128},
   Abstract = {A measurement of the ZZ production cross section in
             proton-proton collisions at √ = 7 TeV using data recorded
             by the ATLAS experiment at the Large Hadron Collider is
             presented. In a data sample corresponding to an integrated
             luminosity of 4.6 fb-1 collected in 2011, events are
             selected that are consistent either with two Z bosons
             decaying to electrons or muons or with one Z boson decaying
             to electrons or muons and a second Z boson decaying to
             neutrinos. The ZZ → ℓ + ℓ - ℓ ′+ ℓ ′- and ZZ
             → ℓ + ℓ - ℓv̄v cross sections are measured in
             restricted phase-space regions. These results are then used
             to derive the total cross section for ZZ events produced
             with both Z bosons in the mass range 66 to 116 GeV, σZZtot
             = 6.7 ± 0.7 (stat.) -0.3+0.4 (stat.) ± 0.3 (lumi.) pb,
             which is consistent with the Standard Model prediction of
             5.89-0.18+0.22 pb calculated at next-to-leading order in
             QCD. The normalized differential cross sections in bins of
             various kinematic variables are presented. Finally, the
             differential event yield as a function of the transverse
             momentum of the leading Z boson is used to set limits on
             anomalous neutral triple gauge boson couplings in ZZ
             production. © 2013 Cern for the benefit of the ATLAS
             collaboration.},
   Doi = {10.1007/JHEP03(2013)128},
   Key = {fds307618}
}

@article{fds356570,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
             Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
             NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
             J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP},
   Title = {Measurement of ZZ production in the ℓℓνν final state
             with the ATLAS detector in pp collisions at √s = 13
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {10},
   Year = {2019},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2019)127},
   Abstract = {This paper presents a measurement of ZZ production with the
             ATLAS detector at the Large Hadron Collider. The measurement
             is carried out in the final state with two charged leptons
             and two neutrinos, using data collected during 2015 and 2016
             in pp collisions at s = 13 TeV, corresponding to an
             integrated luminosity of 36.1 fb−1. The integrated
             cross-sections in the total and fiducial phase spaces are
             measured with an uncertainty of 7% and compared with
             Standard Model predictions, and differential measurements in
             the fiducial phase space are reported. No significant
             deviations from the Standard Model predictions are observed,
             and stringent constraints are placed on anomalous couplings
             corresponding to neutral triple gauge-boson interactions.
             [Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP10(2019)127},
   Key = {fds356570}
}

@article{fds374030,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
             A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport, PP and Aloisio,
             A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev,
             V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
             Ferraz, V and Arcangeletti, C and Arce, ATH and Arena,
             E},
   Title = {Measurement of Zγγ production in pp collisions at √s=13
             TeV with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {6},
   Year = {2023},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11579-8},
   Abstract = {Cross-sections for the production of a Z boson in
             association with two photons are measured in proton–proton
             collisions at a centre-of-mass energy of 13 TeV. The data
             used correspond to an integrated luminosity of 139 fb - 1
             recorded by the ATLAS experiment during Run 2 of the LHC.
             The measurements use the electron and muon decay channels of
             the Z boson, and a fiducial phase-space region where the
             photons are not radiated from the leptons. The integrated
             Z(→ ℓℓ) γγ cross-section is measured with a
             precision of 12% and differential cross-sections are
             measured as a function of six kinematic variables of the
             Zγγ system. The data are compared with predictions from MC
             event generators which are accurate to up to next-to-leading
             order in QCD. The cross-section measurements are used to set
             limits on the coupling strengths of dimension-8 operators in
             the framework of an effective field theory.},
   Doi = {10.1140/epjc/s10052-023-11579-8},
   Key = {fds374030}
}

@article{fds307769,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi,
             E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
             J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
             PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana,
             S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
             J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas,
             CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
             X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ},
   Title = {Measurement of [Formula: see text] production with a veto on
             additional central jet activity in pp collisions at
             [Formula: see text] TeV using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {72},
   Number = {6},
   Pages = {2043},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2043-9},
   Abstract = {A measurement of the jet activity in [Formula: see text]
             events produced in proton-proton collisions at a
             centre-of-mass energy of 7 TeV is presented, using
             2.05 fb<sup>-1</sup> of integrated luminosity collected by
             the ATLAS detector at the Large Hadron Collider. The
             [Formula: see text] events are selected in the dilepton
             decay channel with two identified <i>b</i>-jets from the top
             quark decays. Events are vetoed if they contain an
             additional jet with transverse momentum above a threshold in
             a central rapidity interval. The fraction of events
             surviving the jet veto is presented as a function of this
             threshold for four different central rapidity interval
             definitions. An alternate measurement is also performed, in
             which events are vetoed if the scalar transverse momentum
             sum of the additional jets in each rapidity interval is
             above a threshold. In both measurements, the data are
             corrected for detector effects and compared to the
             theoretical models implemented in MC@NLO, Powheg, Alpgen and
             Sherpa. The experimental uncertainties are often smaller
             than the spread of theoretical predictions, allowing
             deviations between data and theory to be observed in some
             regions of phase space.},
   Doi = {10.1140/epjc/s10052-012-2043-9},
   Key = {fds307769}
}

@article{fds308073,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
             M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
             MA},
   Title = {Measurement of σ(pp̄→Z)•B(Z→ττ) in pp̄ collisions
             at s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {75},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.092004},
   Abstract = {We present a measurement of the inclusive production cross
             section for Z bosons decaying to tau leptons in pp̄
             collisions at s=1.96TeV. We use a channel with one
             hadronically-decaying and one electronically-decaying tau.
             This measurement is based on 350pb-1 of CDF Run II data.
             Using a sample of 504 opposite sign eτ events with a total
             expected background of 190 events, we obtain
             σ(pp̄→4Z)•B(Z→ττ)=264±23(stat)
             ±14(syst)±15(lumi)pb, in agreement with the
             next-to-next-to- leading order QCD prediction. This is the
             first CDF cross section measurement using
             hadronically-decaying taus in Run II. © 2007 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.75.092004},
   Key = {fds308073}
}

@article{fds344668,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
             M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully,
             JC and Cyr, D and Daronco, S and Datta, M and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher,
             A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and Dituro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube,
             S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
             I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Gimmell, JL and Ginsburg,
             C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
             RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
             A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
             S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee,
             SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
             D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
             P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino,
             C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
             M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt,
             J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman,
             J and Nagano, A and Naganoma, J and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
             A and Ranjan, N and Rappoccio, S and Reisert, B and Rekovic, V and Renton,
             P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P},
   Title = {Measurement of σχc2B(χc2→J/ψγ)/ σχc1B(χc1→J/ψγ)
             in pp̄ Collisions at s=1.96TeV},
   Journal = {Physical Review Letters},
   Volume = {98},
   Number = {23},
   Pages = {232001},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.98.232001},
   Abstract = {We measure the ratio of cross section times branching
             fraction, Rp=σχc2B(χc2→J/ψγ)/σχc1B(χc1→J/ ψγ),
             in 1.1fb-1 of pp̄ collisions at s=1.96TeV. This measurement
             covers the kinematic range pT(J/ψ)&gt;4.0GeV/c,
             η(J/ψ)&lt;1.0, and pT(γ)&gt;1.0GeV/c. For events due to
             prompt processes, we find Rp=0.395±0.016(stat)±0.015(syst).
             This result represents a significant improvement in
             precision over previous measurements of prompt χc1,2 hadro
             production. © 2007 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.98.232001},
   Key = {fds344668}
}

@article{fds347471,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
             C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
             AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
             R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
             JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
   Title = {Measurement of τ polarisation in Z / γ ∗ → τ τ
             decays in proton-proton collisions at s = 8 TeV with the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {2},
   Pages = {163},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-5619-1},
   Abstract = {This paper presents a measurement of the polarisation of τ
             leptons produced in Z / γ ∗ → τ τ decays which is
             performed with a dataset of proton-proton collisions at s =
             8 TeV, corresponding to an integrated luminosity of 20.2 fb
             - 1 recorded with the ATLAS detector at the LHC in 2012. The
             Z / γ ∗ → τ τ decays are reconstructed from a
             hadronically decaying τ lepton with a single charged
             particle in the final state, accompanied by a τ lepton that
             decays leptonically. The τ polarisation is inferred from
             the relative fraction of energy carried by charged and
             neutral hadrons in the hadronic τ decays. The polarisation
             is measured in a fiducial region that corresponds to the
             kinematic region accessible to this analysis. The τ
             polarisation extracted over the full phase space within the
             Z / γ ∗ mass range of 66 < m Z / γ ∗ < 116 GeV is
             found to be P τ = - 0.14 ± 0.02 ( stat ) ± 0.04 ( syst )
             . It is in agreement with the Standard Model prediction of P
             τ = - 0.1517 ± 0.0019 , which is obtained from the ALPGEN
             event generator interfaced with the PYTHIA 6 parton shower
             modelling and the TAUOLA τ decay library.},
   Doi = {10.1140/epjc/s10052-018-5619-1},
   Key = {fds347471}
}

@article{fds325306,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
             E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
             N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Da Barreiro Guimarães Costa and J and Bartoldus,
             R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat,
             P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes,
             GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
             V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
             J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
             P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger,
             K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and De Bruckman Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burghgrave,
             B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey,
             P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar,
             CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
             B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and El Cherkaoui Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Chouridou, S and Chow, BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M},
   Title = {Measurement of χc1 and ψχc2 production with √s = 7 TeV
             pp collisions at ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {7},
   Pages = {1-51},
   Publisher = {Springer Verlag},
   Year = {2014},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2014)154},
   Abstract = {The prompt and non-prompt production cross-sections for the
             χc1 and χc2 charmonium states are measured in pp
             collisions at √s = 7TeV with the ATLAS detector at the LHC
             using 4.5 fb−1 of integrated luminosity. The χc states
             are reconstructed through the radiative decay χc → J/ψγ
             (with J/ψ → μ+μ−) where photons are reconstructed
             from γ → e+e− conversions. The production rate of the
             χc2 state relative to the χc1 state is measured for prompt
             and non-prompt χc as a function of J/ψ transverse
             momentum. The prompt χc cross-sections are combined with
             existing measurements of prompt J/ψ production to derive
             the fraction of prompt J/ψ produced in feed-down from χc
             decays. The fractions of χc1 and χc2 produced in b-hadron
             decays are also measured.},
   Doi = {10.1007/JHEP07(2014)154},
   Key = {fds325306}
}

@article{fds308172,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
   Title = {Measurement with the ATLAS detector of multi-particle
             azimuthal correlations in p + Pb collisions at
             √sNN= 5.02 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {725},
   Number = {1-3},
   Pages = {60-78},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.06.057},
   Abstract = {In order to study further the long-range correlations
             ("ridge") observed recently in p + Pb collisions at √sNN=
             5.02 TeV, the second-order azimuthal anisotropy parameter of
             charged particles, v2, has been measured with the cumulant
             method using the ATLAS detector at the LHC. In a data sample
             corresponding to an integrated luminosity of approximately 1
             μb-1, the parameter v2has been obtained using two- and
             four-particle cumulants over the pseudorapidity range
             |η|<2.5. The results are presented as a function of
             transverse momentum and the event activity, defined in terms
             of the transverse energy summed over 3.1 < η <4.9 in the
             direction of the Pb beam. They show features characteristic
             of collective anisotropic flow, similar to that observed in
             Pb + Pb collisions. A comparison is made to results obtained
             using two-particle correlation methods, and to predictions
             from hydrodynamic models of p +Pb collisions. Despite the
             small transverse spatial extent of the p + Pb collision
             system, the large magnitude of v2and its similarity to
             hydrodynamic predictions provide additional evidence for the
             importance of final-state effects in p + Pb reactions. ©
             2013 CERN. Published by Elsevier B.V.},
   Doi = {10.1016/j.physletb.2013.06.057},
   Key = {fds308172}
}

@article{fds356669,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A},
   Title = {Measurements of b-jet tagging efficiency with the ATLAS
             detector using tt¯ events at √s=13 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {8},
   Year = {2018},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2018)089},
   Abstract = {The efficiency to identify jets containing b-hadrons
             (b-jets) is measured using a high purity sample of
             dileptonic top quark-antiquark pairs (tt¯) selected from
             the 36.1 fb−1 of data collected by the ATLAS detector in
             2015 and 2016 from proton-proton collisions produced by the
             Large Hadron Collider at a centre-of-mass energy s=13 TeV.
             Two methods are used to extract the efficiency from tt¯
             events, a combinatorial likelihood approach and a
             tag-and-probe method. A boosted decision tree, not using
             b-tagging information, is used to select events in which two
             b-jets are present, which reduces the dominant uncertainty
             in the modelling of the flavour of the jets. The efficiency
             is extracted for jets in a transverse momentum range from 20
             to 300 GeV, with data-to-simulation scale factors calculated
             by comparing the efficiency measured using collision data to
             that predicted by the simulation. The two methods give
             compatible results, and achieve a similar level of
             precision, measuring data-to-simulation scale factors close
             to unity with uncertainties ranging from 2% to 12% depending
             on the jet transverse momentum.},
   Doi = {10.1007/JHEP08(2018)089},
   Key = {fds356669}
}

@article{fds307888,
   Author = {Aaltonen, and T, and others},
   Title = {Measurements of branching fraction ratios and
             $CP$-asymmetries in suppressed ${B}^{-}\rightarrow
             D(\rightarrow{K}^{+}{\pi}^{-}){K}^{-}$ and
             ${B}^{-}\rightarrow D(\rightarrow{K}^{+} \pi^{-}){\pi}^{-}$
             decays},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {9},
   Pages = {091504},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.091504},
   Abstract = {We report the first reconstruction in hadron collisions of
             the suppressed decays B-→D(→K+π-)K- and
             B-→D(→K+π-)π-, sensitive to the Cabibbo-Kobayashi-Maskawa
             phase γ, using data from 7  fb-1 of integrated
             luminosity collected by the CDF II detector at the Tevatron
             collider. We reconstruct a signal for the B-→D(→K+π-)K-
             suppressed mode with a significance of 3.2 standard
             deviations, and measure the ratios of the suppressed to
             favored branching fractions R(K)=[22.0$\pm$8.6(stat)$\pm$2.6(syst)]×10-3,
             R+(K)=[42.6$\pm$13.7(stat)$\pm$2.8(syst)]×10-3,
             R-(K)=[3.8$\pm$10.3(stat)$\pm$2.7(syst)]×10-3 as well as
             the direct CP-violating asymmetry A(K)=-0.82$\pm$0.44(stat)$\pm$0.09(syst)
             of this mode. Corresponding quantities for
             B-→D(→K+π-)π- decay are also reported.},
   Doi = {10.1103/PhysRevD.84.091504},
   Key = {fds307888}
}

@article{fds307926,
   Author = {Aaltonen, and T, and others},
   Title = {Measurements of branching fraction ratios and CP asymmetries
             in $B^\pm \to D_{CP} K^\pm$ decays in hadron
             collisions},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {3},
   Pages = {031105},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.031105},
   Abstract = {http://arxiv.org/abs/0911.0425},
   Doi = {10.1103/PhysRevD.81.031105},
   Key = {fds307926}
}

@article{fds356763,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
             H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurements of charge and CP asymmetries in b-hadron decays
             using top-quark events collected by the ATLAS detector in pp
             collisions at √s=8 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {2},
   Year = {2017},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP02(2017)071},
   Abstract = {Same- and opposite-sign charge asymmetries are measured in
             lepton+jets tt¯ events in which a b-hadron decays
             semileptonically to a soft muon, using data corresponding to
             an integrated luminosity of 20.3 fb−1 from proton-proton
             collisions at a centre-of-mass energy of s=√8 TeV
             collected with the ATLAS detector at the Large Hadron
             Collider at CERN. The charge asymmetries are based on the
             charge of the lepton from the top-quark decay and the charge
             of the soft muon from the semileptonic decay of a b-hadron
             and are measured in a fiducial region corresponding to the
             experimental acceptance. Four CP asymmetries (one mixing and
             three direct) are measured and are found to be compatible
             with zero and consistent with the Standard Model.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP02(2017)071},
   Key = {fds356763}
}

@article{fds374213,
   Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
             BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
             P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez, AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Dos Santos and SPA and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
   Title = {Measurements of differential cross sections of Higgs boson
             production through gluon fusion in the H? WW*?
             e?µ? final state at √s=13 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {9},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2023},
   Month = {September},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11873-5},
   Abstract = {Higgs boson production via gluon–gluon fusion is measured
             in the WW*? e?µ? decay channel. The dataset utilized
             corresponds to an integrated luminosity of 139 fb - 1
             collected by the ATLAS detector from s=13 TeV
             proton–proton collisions delivered by the Large Hadron
             Collider between 2015 and 2018. Differential cross sections
             are measured in a fiducial phase space restricted to the
             production of at most one additional jet. The results are
             consistent with Standard Model expectations, derived using
             different Monte Carlo generators.},
   Doi = {10.1140/epjc/s10052-023-11873-5},
   Key = {fds374213}
}

@article{fds356657,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada
             Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A},
   Title = {Measurements of differential cross sections of top quark
             pair production in association with jets in pp collisions at
             √s=13 TeV using the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {10},
   Year = {2018},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2018)159},
   Abstract = {Measurements of differential cross sections of top quark
             pair production in association with jets by the ATLAS
             experiment at the LHC are presented. The measurements are
             performed as functions of the top quark transverse momentum,
             the transverse momentum of the top quark-antitop quark
             system and the out-of-plane transverse momentum using data
             from pp collisions at s=13 TeV collected by the ATLAS
             detector at the LHC in 2015 and corresponding to an
             integrated luminosity of 3.2 fb−1. The top quark pair
             events are selected in the lepton (electron or muon) + jets
             channel. The measured cross sections, which are compared to
             several predictions, allow a detailed study of top quark
             production.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP10(2018)159},
   Key = {fds356657}
}

@article{fds357655,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
             C},
   Title = {Measurements of differential cross-sections in four-lepton
             events in 13 TeV proton-proton collisions with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {7},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2021)005},
   Abstract = {Measurements of four-lepton differential and integrated
             fiducial cross-sections in events with two same-flavour,
             opposite-charge electron or muon pairs are presented. The
             data correspond to 139 fb−1 of s = 13 TeV proton-proton
             collisions, collected by the ATLAS detector during Run 2 of
             the Large Hadron Collider (2015–2018). The final state has
             contributions from a number of interesting Standard Model
             processes that dominate in different four-lepton invariant
             mass regions, including single Z boson production, Higgs
             boson production and on-shell ZZ production, with a complex
             mix of interference terms, and possible contributions from
             physics beyond the Standard Model. The differential
             cross-sections include the four-lepton invariant mass
             inclusively, in slices of other kinematic variables, and in
             different lepton flavour categories. Also measured are
             dilepton invariant masses, transverse momenta, and angular
             correlation variables, in four regions of four-lepton
             invariant mass, each dominated by different processes. The
             measurements are corrected for detector effects and are
             compared with state-of-the-art Standard Model calculations,
             which are found to be consistent with the data. The Z →
             4ℓ branching fraction is extracted, giving a value of
             (4.41 ± 0.30) × 10−6. Constraints on effective field
             theory parameters and a model based on a spontaneously
             broken B − L gauge symmetry are also evaluated. Further
             reinterpretations can be performed with the provided
             information. [Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP07(2021)005},
   Key = {fds357655}
}

@article{fds307847,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurements of Direct ${CP}$ Violating Asymmetries in
             Charmless Decays of Strange Bottom Mesons and Bottom
             Baryons},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {18},
   Pages = {181802},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.181802},
   Abstract = {We report measurements of direct CP-violating asymmetries in
             charmless decays of neutral bottom hadrons to pairs of
             charged hadrons with the upgraded Collider Detector at the
             Fermilab Tevatron. Using a data sample corresponding to 1
             fb(-1) of integrated luminosity, we obtain the first
             measurements of direct CP violation in bottom strange
             mesons, A(CP)(B(s)(0)→K(-)π(+))=+0.39±0.15(stat)±0.08(syst),
             and bottom baryons, A(CP)(Λ(b)(0)→pπ(-))=+0.03±0.17(stat)±0.05(syst)
             and A(CP)(Λ(b)(0)→pK(-))=+0.37±0.17(stat)±0.03(syst).
             In addition, we measure CP violation in B(0)→K(+)π(-)
             decays with 3.5σ significance, A(CP)(B(0)→K(+)π(-))=-0.086±0.023(stat)±0.009(syst),
             in agreement with the current world average. Measurements of
             branching fractions of B(s)(0)→K(+)K(-) and
             B(0)→π(+)π(-) decays are also updated.},
   Doi = {10.1103/PhysRevLett.106.181802},
   Key = {fds307847}
}

@article{fds346169,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
             JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
             A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
             C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
             L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Measurements of direct CP-violating asymmetries in charmless
             decays of bottom baryons.},
   Journal = {Physical review letters},
   Volume = {113},
   Number = {24},
   Pages = {242001},
   Year = {2014},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.113.242001},
   Abstract = {We report final measurements of direct CP-violating
             asymmetries in charmless decays of neutral bottom hadrons to
             pairs of charged hadrons with the upgraded Collider Detector
             at the Fermilab Tevatron. Using the complete
             √s=1.96  TeV proton-antiproton collisions data set,
             corresponding to 9.3  fb⁻¹ of integrated luminosity,
             we measure A(Λ(b)⁰→pπ⁻)=+0.06±0.07(stat)±0.03(syst)
             and A(Λ(b)⁰→pK⁻)=-0.10±0.08(stat)±0.04(syst),
             compatible with no asymmetry. In addition we measure the
             CP-violating asymmetries in B(s)⁰→K⁻π⁺ and
             B⁰→K⁺π⁻ decays to be A(B(s)⁰→K⁻π⁺)=+0.22±0.07(stat)±0.02(syst)
             and A(B⁰→K⁺π⁻)=-0.083±0.013(stat)±0.004(syst),
             respectively, which are significantly different from zero
             and consistent with current world averages.},
   Doi = {10.1103/physrevlett.113.242001},
   Key = {fds346169}
}

@article{fds347507,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
             M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Piqueras,
             DÁ and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung,
             C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and da Costa, JBG and Bartoldus,
             R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates,
             RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer,
             F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin,
             PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski,
             R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Billoud,
             TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard,
             J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger,
             AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr,
             JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
             JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Bret, MC and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrillo-Montoya, GD and Carvalho, J and Casadei,
             D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
             E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito,
             L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez
             Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
             S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
             YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
             BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL and Clark, MR and Clark,
             PJ},
   Title = {Measurements of electroweak [Formula: see text] production
             and constraints on anomalous gauge couplings with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {7},
   Pages = {474},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5007-2},
   Abstract = {Measurements of the electroweak production of a <i>W</i>
             boson in association with two jets at high dijet invariant
             mass are performed using [Formula: see text] 7 and
             8 [Formula: see text] proton-proton collision data
             produced by the Large Hadron Collider, corresponding
             respectively to 4.7 and 20.2 fb[Formula: see text] of
             integrated luminosity collected by the ATLAS detector. The
             measurements are sensitive to the production of a <i>W</i>
             boson via a triple-gauge-boson vertex and include both the
             fiducial and differential cross sections of the electroweak
             process.},
   Doi = {10.1140/epjc/s10052-017-5007-2},
   Key = {fds347507}
}

@article{fds313591,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurements of fiducial and differential cross sections for
             Higgs boson production in the diphoton decay channel at √s
             = 8 TeV with ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {9},
   Pages = {1-60},
   Year = {2014},
   Month = {September},
   ISSN = {1126-6708},
   url = {http://dx.doi.org/10.1007/JHEP09(2014)112},
   Abstract = {Measurements of fiducial and differential cross sections are
             presented for Higgs boson production in proton-proton
             collisions at a centre-of-mass energy of √s = 8TeV. The
             analysis is performed in the H → γγ decay channel using
             20.3 fb−1 of data recorded by the ATLAS experiment at the
             CERN Large Hadron Collider. The signal is extracted using a
             fit to the diphoton invariant mass spectrum assuming that
             the width of the resonance is much smaller than the
             experimental resolution. The signal yields are corrected for
             the effects of detector inefficiency and resolution. The pp
             → H → γγ fiducial cross section is measured to be 43.2
             ±9.4 (stat.) +3.2−2.9 (syst.) ±1.2 (lumi) fb for a Higgs
             boson of mass 125.4 GeV decaying to two isolated photons
             that have transverse momentum greater than 35% and 25% of
             the diphoton invariant mass and each with absolute
             pseudorapidity less than 2.37. Four additional fiducial
             cross sections and two cross-section limits are presented in
             phase space regions that test the theoretical modelling of
             different Higgs boson production mechanisms, or are
             sensitive to physics beyond the Standard Model. Differential
             cross sections are also presented, as a function of
             variables related to the diphoton kinematics and the jet
             activity produced in the Higgs boson events. The observed
             spectra are statistically limited but broadly in line with
             the theoretical expectations.},
   Doi = {10.1007/JHEP09(2014)112},
   Key = {fds313591}
}

@article{fds346162,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
             M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
             C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
             A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P},
   Title = {Measurements of fiducial cross-sections for [Formula: see
             text] production with one or two additional b-jets in
             pp collisions at [Formula: see text]=8 TeV using the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {11},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3852-4},
   Abstract = {Fiducial cross-sections for [Formula: see text] production
             with one or two additional <i>b</i>-jets are reported, using
             an integrated luminosity of 20.3 fb[Formula: see text] of
             proton-proton collisions at a centre-of-mass energy of 8
             TeV at the Large Hadron Collider, collected with the ATLAS
             detector. The cross-section times branching ratio for
             [Formula: see text] events with at least one additional
             <i>b</i>-jet is measured to be 950 [Formula: see text]
             70 (stat.) [Formula: see text] (syst.) fb in the
             lepton-plus-jets channel and 50 [Formula: see text]
             10 (stat.) [Formula: see text] (syst.) fb in the
             [Formula: see text] channel. The cross-section times
             branching ratio for events with at least two additional
             <i>b</i>-jets is measured to be 19.3 [Formula: see text]
             3.5 (stat.) [Formula: see text] 5.7 (syst.) fb in the
             dilepton channel ([Formula: see text], [Formula: see text],
             and  <i>ee</i>) using a method based on tight selection
             criteria, and 13.5 [Formula: see text] 3.3 (stat.) [Formula:
             see text] 3.6 (syst.) fb using a looser selection that
             allows the background normalisation to be extracted from
             data. The latter method also measures a value of 1.30
             [Formula: see text] 0.33 (stat.) [Formula: see text]
             0.28 (syst.)% for the ratio of [Formula: see text]
             production with two additional <i>b</i>-jets to [Formula:
             see text] production with any two additional jets. All
             measurements are in good agreement with recent theory
             predictions.},
   Doi = {10.1140/epjc/s10052-015-3852-4},
   Key = {fds346162}
}

@article{fds307530,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Asman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai,
             Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JC and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC},
   Title = {Measurements of four-lepton production at the Z resonance in
             pp collisions at sqrt[s] = 7 and 8 TeV with
             ATLAS.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {23},
   Pages = {231806},
   Year = {2014},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.112.231806},
   Abstract = {Measurements of four-lepton (4ℓ, ℓ=e,μ) production
             cross sections at the Z resonance in pp collisions at the
             LHC with the ATLAS detector are presented. For dilepton and
             four-lepton invariant mass regions m(ℓ+ℓ(-)) > 5 GeV and
             80<m(4ℓ) < 100 GeV, the measured cross sections are 76 ±
             18(stat) ± 4(syst) ± 1.4(lumi) fb and 107 ± 9(stat) ±
             4(syst) ± 3.0(lumi) fb at sqrt[s] = 7 and 8 TeV,
             respectively. By subtracting the nonresonant 4ℓ production
             contributions and normalizing with Z → μ(+)μ(-) events,
             the branching fraction for the Z boson decay to 4ℓ is
             determined to be (3.20 ± 0.25(stat) ± 0.13(syst)) ×
             10(-6), consistent with the standard model
             prediction.},
   Doi = {10.1103/physrevlett.112.231806},
   Key = {fds307530}
}

@article{fds356782,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Measurements of four-lepton production in pp collisions at
             √s=8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {753},
   Pages = {552-572},
   Year = {2016},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.12.048},
   Abstract = {The four-lepton (4ℓ, ℓ=e,μ) production cross section is
             measured in the mass range from 80 to 1000 GeV using 20.3
             fb−1 of data in pp collisions at s=8 TeV collected with
             the ATLAS detector at the LHC. The 4ℓ events are produced
             in the decays of resonant Z and Higgs bosons and the
             non-resonant ZZ continuum originating from qq¯, gg, and qg
             initial states. A total of 476 signal candidate events are
             observed with a background expectation of 26.2±3.6 events,
             enabling the measurement of the integrated cross section and
             the differential cross section as a function of the
             invariant mass and transverse momentum of the four-lepton
             system. In the mass range above 180 GeV, assuming the
             theoretical constraint on the qq¯ production cross section
             calculated with perturbative NNLO QCD and NLO electroweak
             corrections, the signal strength of the gluon-fusion
             component relative to its leading-order prediction is
             determined to be μgg=2.4±1.0 (stat.)±0.5 (syst.)±0.8
             (theory).},
   Doi = {10.1016/j.physletb.2015.12.048},
   Key = {fds356782}
}

@article{fds347553,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {Measurements of gluon–gluon fusion and vector-boson fusion
             Higgs boson production cross-sections in the
             H → WW → eνμν decay channel in
             pp collisions at √s=13TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {789},
   Pages = {508-529},
   Year = {2019},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.11.064},
   Abstract = {Higgs boson production cross-sections in proton–proton
             collisions are measured in the H→WW⁎→eνμν decay
             channel. The proton–proton collision data were produced at
             the Large Hadron Collider at a centre-of-mass energy of 13
             TeV and recorded by the ATLAS detector in 2015 and 2016,
             corresponding to an integrated luminosity of 36.1fb−1. The
             product of the H→WW⁎ branching fraction times the
             gluon–gluon fusion and vector-boson fusion cross-sections
             are measured to be 11.4−1.1+1.2(stat.)−1.7+1.8(syst.)pb
             and 0.50−0.22+0.24(stat.)±0.17(syst.)pb, respectively, in
             agreement with Standard Model predictions.},
   Doi = {10.1016/j.physletb.2018.11.064},
   Key = {fds347553}
}

@article{fds307582,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and AbdelKhalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
             M},
   Title = {Measurements of Higgs boson production and couplings in
             diboson final states with the ATLAS detector at the
             LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {726},
   Number = {1-3},
   Pages = {88-119},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.08.010},
   Abstract = {Measurements are presented of production properties and
             couplings of the recently discovered Higgs boson using the
             decays into boson pairs, H→γγ, H→ZZ*→4ℓ and
             H→WW*→ℓνℓν. The results are based on the complete
             pp collision data sample recorded by the ATLAS experiment at
             the CERN Large Hadron Collider at centre-of-mass energies of
             s=7 TeV and s=8 TeV, corresponding to an integrated
             luminosity of about 25 fb-1. Evidence for Higgs boson
             production through vector-boson fusion is reported. Results
             of combined fits probing Higgs boson couplings to fermions
             and bosons, as well as anomalous contributions to
             loop-induced production and decay modes, are presented. All
             measurements are consistent with expectations for the
             Standard Model Higgs boson. © 2013 CERN.},
   Doi = {10.1016/j.physletb.2013.08.010},
   Key = {fds307582}
}

@article{fds310326,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H},
   Title = {Measurements of Higgs boson production and couplings in the
             four-lepton channel in pp collisions at center-of-mass
             energies of 7 and 8 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.012006},
   Abstract = {The final ATLAS Run 1 measurements of Higgs boson production
             and couplings in the decay channel H → ZZ∗ →
             l+l-l'+l'-, where l, l' = e or μ, are presented. These
             measurements were performed using pp collision data
             corresponding to integrated luminosities of 4.5 and 20.3
             fb-1 at center-of-mass energies of 7 and 8 TeV,
             respectively, recorded with the ATLAS detector at the LHC.
             The H → ZZ∗ → 4l signal is observed with a
             significance of 8.1 standard deviations, with an expectation
             of 6.2 standard deviations, at mH = 125.36 GeV, the combined
             ATLAS measurement of the Higgs boson mass from the H →
             γγ and H → ZZ∗ → 4l channels. The production rate
             relative to the Standard Model expectation, the signal
             strength, is measured in four different production
             categories in the H → ZZ∗ → 4l channel. The measured
             signal strength, at this mass, and with all categories
             combined, is 1.44+0.40-0.33. The signal strength for Higgs
             boson production in gluon fusion or in association with tt
             or bb pairs is found to be 1.7+0.5-0.4, while the signal
             strength for vector-boson fusion combined with WH/ZH
             associated production is found to be 0.3+1.6-0.9.},
   Doi = {10.1103/PhysRevD.91.012006},
   Key = {fds310326}
}

@article{fds373465,
   Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Franco, L and Goy, C and Guillemin,
             T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben,
             M and Bouquet, R and Marchiori, G and Bhopatkar, VS and Chekanov, S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
             Gemmeren, P and Wang, R and Zhang, J and Berlendis, S and Cheu, E and Cui,
             Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta,
             D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand,
             HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Unal, M and Webb, AF and Huseynov, N and Agaras, MN and Bogavac, D and Bosman, M},
   Title = {Measurements of Higgs boson production by gluon-gluon fusion
             and vector-boson fusion using H→WW*→eνμν decays in pp
             collisions at Formula Presented with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {108},
   Number = {3},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.108.032005},
   Abstract = {Higgs boson production via gluon-gluon fusion and
             vector-boson fusion in proton-proton collisions is measured
             in the H → W W * → e ν μ ν decay channel. The Large
             Hadron Collider delivered proton-proton collisions at a
             center-of-mass energy of 13 TeV between 2015 and 2018, which
             were recorded by the ATLAS detector, corresponding to an
             integrated luminosity of 139 fb - 1 . The total cross
             sections for Higgs boson production by gluon-gluon fusion
             and vector-boson fusion times the H → W W * branching
             ratio are measured to be 12.0 ± 1.4 and 0.75 - 0.16 + 0.19
             pb , respectively, in agreement with the Standard Model
             predictions of 10.4 ± 0.6 and 0.81 ± 0.02 pb . Higgs boson
             production is further characterized through measurements of
             Simplified Template Cross Sections in a total of 11
             kinematic fiducial regions.},
   Doi = {10.1103/PhysRevD.108.032005},
   Key = {fds373465}
}

@article{fds356660,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
             P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Measurements of Higgs boson properties in the diphoton decay
             channel with 36 fb -1 of pp collision data at
             √s = 13 TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {5},
   Year = {2018},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.052005},
   Abstract = {Properties of the Higgs boson are measured in the two-photon
             final state using 36.1 fb-1 of proton? proton collision data
             recorded at ffiffi √s = 13 TeV by the ATLAS experiment at
             the Large Hadron Collider. Cross-section measurements for
             the production of a Higgs boson through gluon-gluon fusion,
             vectorboson fusion, and in association with a vector boson
             or a top-quark pair are reported. The signal strength,
             defined as the ratio of the observed to the expected signal
             yield, is measured for each of these production processes as
             well as inclusively. The global signal strength measurement
             of 0.99 ± 0.14 improves on the precision of the ATLAS
             measurement at √s = 7 and 8 TeV by a factor of two.
             Measurements of gluon-gluon fusion and vector-boson fusion
             productions yield signal strengths compatible with the
             Standard Model prediction. Measurements of simplified
             template cross sections, designed to quantify the different
             Higgs boson production processes in specific regions of
             phase space, are reported. The cross section for the
             production of the Higgs boson decaying to two isolated
             photons in a fiducial region closely matching the
             experimental selection of the photons is measured to be 55
             ± 10 fb, which is in good agreement with the Standard Model
             prediction of 64 ± 2 fb. Furthermore, cross sections in
             fiducial regions enriched in Higgs boson production in
             vector-boson fusion or in association with large missing
             transverse momentum, leptons or top-quark pairs are
             reported. Differential and double-differential measurements
             are performed for several variables related to the diphoton
             kinematics as well as the kinematics and multiplicity of the
             jets produced in association with a Higgs boson. These
             differential cross sections are sensitive to higher order
             QCD corrections and properties of the Higgs boson, such as
             its spin and CP quantum numbers. No significant deviations
             from a wide array of Standard Model predictions are
             observed. Finally, the strength and tensor structure of the
             Higgs boson interactions are investigated using an effective
             Lagrangian, which introduces additional CP-even and CP-odd
             interactions. No significant new physics contributions are
             observed.},
   Doi = {10.1103/PhysRevD.98.052005},
   Key = {fds356660}
}

@article{fds357500,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
             J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
             C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C and Arce, ATH and Arguin, JF},
   Title = {Measurements of Higgs bosons decaying to bottom quarks from
             vector boson fusion production with the ATLAS experiment at
             √s=13TeV},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {6},
   Year = {2021},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09192-8},
   Abstract = {The paper presents a measurement of the Standard Model Higgs
             Boson decaying to b-quark pairs in the vector boson fusion
             (VBF) production mode. A sample corresponding to 126 fb - 1
             of s=13TeV proton–proton collision data, collected with
             the ATLAS experiment at the Large Hadron Collider, is
             analyzed utilizing an adversarial neural network for event
             classification. The signal strength, defined as the ratio of
             the measured signal yield to that predicted by the Standard
             Model for VBF Higgs production, is measured to be
             0.95-0.36+0.38 , corresponding to an observed (expected)
             significance of 2.6 (2.8) standard deviations from the
             background only hypothesis. The results are additionally
             combined with an analysis of Higgs bosons decaying to
             b-quarks, produced via VBF in association with a
             photon.},
   Doi = {10.1140/epjc/s10052-021-09192-8},
   Key = {fds357500}
}

@article{fds352489,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {Measurements of inclusive and differential cross-sections of
             combined tt¯ γ and tWγ production in the eμ channel at
             13 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {9},
   Year = {2020},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2020)049},
   Abstract = {Inclusive and differential cross-sections for the production
             of top quarks in association with a photon are measured with
             proton-proton collision data corresponding to an integrated
             luminosity of 139 fb−1. The data were collected by the
             ATLAS detector at the LHC during Run 2 between 2015 and 2018
             at a centre-of-mass energy of 13 TeV. The measurements are
             performed in a fiducial volume defined at parton level.
             Events with exactly one photon, one electron and one muon of
             opposite sign, and at least two jets, of which at least one
             is b-tagged, are selected. The fiducial cross-section is
             measured to be 39.6−2.3+2.7 fb. Differential
             cross-sections as functions of several observables are
             compared with state-of-the-art Monte Carlo simulations and
             next-to-leading-order theoretical calculations. These
             include cross-sections as functions of photon kinematic
             variables, angular variables related to the photon and the
             leptons, and angular separations between the two leptons in
             the event. All measurements are in agreement with the
             predictions from the Standard Model. [Figure not available:
             see fulltext.]},
   Doi = {10.1007/JHEP09(2020)049},
   Key = {fds352489}
}

@article{fds356611,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {Measurements of inclusive and differential fiducial
             cross-sections of tt¯ production with additional
             heavy-flavour jets in proton-proton collisions at √s = 13
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {4},
   Year = {2019},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2019)046},
   Abstract = {This paper presents measurements of tt¯ production in
             association with additional b-jets in pp collisions at the
             LHC at a centre-of-mass energy of 13 TeV. The data were
             recorded with the ATLAS detector and correspond to an
             integrated luminosity of 36.1 fb −1 . Fiducial
             cross-section measurements are performed in the dilepton and
             lepton-plus-jets tt¯ decay channels. Results are presented
             at particle level in the form of inclusive cross-sections of
             tt¯ final states with three and four b-jets as well as
             differential cross-sections as a function of global event
             properties and properties of b-jet pairs. The measured
             inclusive fiducial cross-sections generally exceed the tt¯
             bb¯ predictions from various next-to-leading-order matrix
             element calculations matched to a parton shower but are
             compatible within the total uncertainties. The experimental
             uncertainties are smaller than the uncertainties in the
             predictions. Comparisons of state-of-the-art theoretical
             predictions with the differential measurements are shown and
             good agreement with data is found for most of them.[Figure
             not available: see fulltext.].},
   Doi = {10.1007/JHEP04(2019)046},
   Key = {fds356611}
}

@article{fds356601,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos,
             SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
             VA and Pereira, RA and Arce, ATH and Ardell, RE and Arduh,
             FA},
   Title = {Measurements of inclusive and differential fiducial
             cross-sections of tt¯ γ production in leptonic final
             states at √s=13TeV in ATLAS},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {5},
   Year = {2019},
   Month = {May},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-6849-6},
   Abstract = {Inclusive and differential cross-sections for the production
             of a top-quark pair in association with a photon are
             measured with proton-proton collision data corresponding to
             an integrated luminosity of 36.1 fb-1, collected by the
             ATLAS detector at the LHC in 2015 and 2016 at a
             centre-of-mass energy of 13 TeV. The measurements are
             performed in single-lepton and dilepton final states in a
             fiducial volume. Events with exactly one photon, one or two
             leptons, a channel-dependent minimum number of jets, and at
             least one b-jet are selected. Neural network algorithms are
             used to separate the signal from the backgrounds. The
             fiducial cross-sections are measured to be
             521±9(stat.)±41(sys.)fb and 69±3(stat.)±4(sys.)fb for
             the single-lepton and dilepton channels, respectively. The
             differential cross-sections are measured as a function of
             photon transverse momentum, photon absolute pseudorapidity,
             and angular distance between the photon and its closest
             lepton in both channels, as well as azimuthal opening angle
             and absolute pseudorapidity difference between the two
             leptons in the dilepton channel. All measurements are in
             agreement with the theoretical predictions.},
   Doi = {10.1140/epjc/s10052-019-6849-6},
   Key = {fds356601}
}

@article{fds308069,
   Author = {Abulencia, A and others},
   Title = {Measurements of Inclusive W and Z Cross Sections in p anti-p
             Collisions at $\sqrt{s} = 1.96$ TeV},
   Journal = {J. Phys. G: Nucl. Part. Phys.},
   Volume = {34},
   Number = {12},
   Pages = {2457-2544},
   Publisher = {IOP Publishing},
   Year = {2007},
   url = {http://dx.doi.org/10.1088/0954-3899/34/12/001},
   Abstract = {We report the first measurements of inclusive W and Z boson
             cross-sections times the corresponding leptonic branching
             ratios for p anti-p collisions at s**(1/2) = 1.96 TeV based
             on the decays of the W and Z bosons into electrons and
             muons. The data were recorded with the CDF II detector at
             the Fermilab Tevatron and correspond to an integrated
             luminosity of 72.0 +/- 4.3 pb-1. We test e-mu lepton
             universality in W decays by measuring the ratio of the W -->
             mu nu to W --> e nu cross sections and determine a value to
             0.991 +/- 0.004(stat.) +/- 0.011(syst.) for the ratio of W -
             l - nu couplings (g_mu/g_e). Since there is no sign of
             non-universality, we combine our cross-section measurements
             in the different lepton decay modes and obtain sigma_W x
             Br(p anti-p --> W --> l nu) = 2.749 +/- 0.010(stat.) +/-
             0.053(syst.) +/- 0.165(lum.) nb and sigma_gamma*/Z x BR(p
             anti-p --> gamma*/Z --> ll) = 254.9 +/- 3.3(stat.) +/-
             4.6(syst.) +/- 15.2(lum.) pb for dilepton pairs in the mass
             range between 66 GeV/c2 and 116 GeV/c2. We compute the ratio
             R of the W --> l nu to Z --> ll cross section taking all
             correlations among channels into account and obtain R =
             10.84 +/- 0.15(stat.) +/- 0.14(syst.) including a correction
             for the virtual photon exchange component in our measured
             gamma*/Z --> ll cross section. Based on the measured value
             of R, we extract values for the W leptonic branching ratio,
             Br(W --> l nu) = 0.1082 +/- 0.0022; the total width of the W
             boson, Gamma(W) = 2092 +/- 42 MeV; and the ratio of W and Z
             boson total widths, Gamma(W)/Gamma(Z) = 0.838 +/- 0.017. In
             addition, we use our extracted value of Gamma(W) whose value
             depends on various electroweak parameters and certain CKM
             matrix elements to constrain the V_cs CKM matrix element,
             |V_cs| = 0.976 +/- 0.030.},
   Doi = {10.1088/0954-3899/34/12/001},
   Key = {fds308069}
}

@article{fds356750,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Measurements of integrated and differential cross sections
             for isolated photon pair production in pp collisions at √
             s = 8 TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {95},
   Number = {11},
   Year = {2017},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.95.112005},
   Abstract = {A measurement of the production cross section for two
             isolated photons in proton-proton collisions at a
             center-of-mass energy of s=8 TeV is presented. The results
             are based on an integrated luminosity of 20.2 fb-1 recorded
             by the ATLAS detector at the Large Hadron Collider. The
             measurement considers photons with pseudorapidities
             satisfying |ηγ|<1.37 or 1.56<|ηγ|<2.37 and transverse
             energies of respectively ET,1γ>40 GeV and ET,2γ>30 GeV for
             the two leading photons ordered in transverse energy
             produced in the interaction. The background due to hadronic
             jets and electrons is subtracted using data-driven
             techniques. The fiducial cross sections are corrected for
             detector effects and measured differentially as a function
             of six kinematic observables. The measured cross section
             integrated within the fiducial volume is 16.8±0.8 pb. The
             data are compared to fixed-order QCD calculations at
             next-to-leading-order and next-to-next-to-leading-order
             accuracy as well as next-to-leading-order computations
             including resummation of initial-state gluon radiation at
             next-to-next-to-leading logarithm or matched to a parton
             shower, with relative uncertainties varying from 5% to
             20%.},
   Doi = {10.1103/PhysRevD.95.112005},
   Key = {fds356750}
}

@article{fds310389,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Bessner, MF and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro,
             A},
   Title = {Measurements of jet vetoes and azimuthal decorrelations in
             dijet events produced in [Formula: see text] collisions at
             [Formula: see text] using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {11},
   Pages = {3117},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3117-7},
   Abstract = {Additional jet activity in dijet events is measured using
             [Formula: see text] collisions at ATLAS at a centre-of-mass
             energy of [Formula: see text], for jets reconstructed using
             the [Formula: see text] algorithm with radius parameter
             [Formula: see text]. This is done using variables such as
             the fraction of dijet events without an additional jet in
             the rapidity interval bounded by the dijet subsystem and
             correlations between the azimuthal angles of the dijet s.
             They are presented, both with and without a veto on
             additional jet activity in the rapidity interval, as a
             function of the scalar average of the transverse momenta of
             the dijet s and of the rapidity interval size. The double
             differential dijet cross section is also measured as a
             function of the interval size and the azimuthal angle
             between the dijet s. These variables probe differences in
             the approach to resummation of large logarithms when
             performing QCD calculations. The data are compared to
             powheg, interfaced to the pythia 8 and herwig parton shower
             generators, as well as to hej with and without interfacing
             it to the ariadne parton shower generator. None of the
             theoretical predictions agree with the data across the full
             phase-space considered; however, powheg+pythia 8 and
             hej+ariadne are found to provide the best agreement with the
             data. These measurements use the full data sample collected
             with the ATLAS detector in [Formula: see text][Formula: see
             text] collisions at the LHC and correspond to integrated
             luminosities of [Formula: see text] and [Formula: see text]
             for data collected during 2010 and 2011,
             respectively.},
   Doi = {10.1140/epjc/s10052-014-3117-7},
   Key = {fds310389}
}

@article{fds356742,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu,
             H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik,
             M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O},
   Title = {Measurements of long-range azimuthal anisotropies and
             associated Fourier coefficients for pp collisions at s =5.02
             and 13 TeV and p+Pb collisions at sNN =5.02 TeV with the
             ATLAS detector},
   Journal = {Physical Review C},
   Volume = {96},
   Number = {2},
   Year = {2017},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevC.96.024908},
   Abstract = {ATLAS measurements of two-particle correlations are
             presented for s=5.02 and 13 TeV pp collisions and for
             sNN=5.02 TeV p+Pb collisions at the LHC. The correlation
             functions are measured as a function of relative azimuthal
             angle Δφ, and pseudorapidity separation Δη, using
             charged particles detected within the pseudorapidity
             interval |η|<2.5. Azimuthal modulation in the long-range
             component of the correlation function, with |Δη|>2, is
             studied using a template fitting procedure to remove a
             "back-to-back" contribution to the correlation function that
             primarily arises from hard-scattering processes. In addition
             to the elliptic, cos(2Δφ), modulation observed in a
             previous measurement, the pp correlation functions exhibit
             significant cos(3Δφ) and cos(4Δφ) modulation. The
             Fourier coefficients vn,n associated with the cos(nΔφ)
             modulation of the correlation functions for n=2-4 are
             measured as a function of charged-particle multiplicity and
             charged-particle transverse momentum. The Fourier
             coefficients are observed to be compatible with cos(nφ)
             modulation of per-event single-particle azimuthal angle
             distributions. The single-particle Fourier coefficients vn
             are measured as a function of charged-particle multiplicity,
             and charged-particle transverse momentum for n=2-4. The
             integrated luminosities used in this analysis are, 64 nb-1
             for the s=13 TeV pp data, 170 nb-1 for the s=5.02 TeV pp
             data, and 28 nb-1 for the sNN=5.02 TeV p+Pb
             data.},
   Doi = {10.1103/PhysRevC.96.024908},
   Key = {fds356742}
}

@article{fds313594,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurements of normalized differential cross sections for
             t¯t production in pp collisions at √(s) = 7 TeV using the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {October},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.072004},
   Abstract = {Measurements of normalized differential cross sections for
             top-quark pair production are presented as a function of the
             top-quark transverse momentum, and of the mass, transverse
             momentum, and rapidity of the t¯t system, in proton-proton
             collisions at a center-of-mass energy of √s = 7 TeV. The
             data set corresponds to an integrated luminosity of 4.6
             fb-1, recorded in 2011 with the ATLAS detector at the CERN
             Large Hadron Collider. Events are selected in the lepton +
             jets channel, requiring exactly one lepton and at least four
             jets with at least one of the jets tagged as originating
             from a b-quark. The measured spectra are corrected for
             detector efficiency and resolution effects and are compared
             to several Monte Carlo simulations and theory calculations.
             The results are in fair agreement with the predictions in a
             wide kinematic range. Nevertheless, data distributions are
             softer than predicted for higher values of the mass of the
             t¯t system and of the top-quark transverse momentum. The
             measurements can also discriminate among different sets of
             parton distribution functions.},
   Doi = {10.1103/PhysRevD.90.072004},
   Key = {fds313594}
}

@article{fds374029,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
             A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
             W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
             MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
   Title = {Measurements of observables sensitive to colour reconnection
             in tt¯ events with the ATLAS detector at √s=
             13 TeV},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {6},
   Year = {2023},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11479-x},
   Abstract = {A measurement of observables sensitive to effects of colour
             reconnection in top-quark pair-production events is
             presented using 139 fb - 1 of 13 TeV proton–proton
             collision data collected by the ATLAS detector at the LHC.
             Events are selected by requiring exactly one isolated
             electron and one isolated muon with opposite charge and two
             or three jets, where exactly two jets are required to be
             b-tagged. For the selected events, measurements are
             presented for the charged-particle multiplicity, the scalar
             sum of the transverse momenta of the charged particles, and
             the same scalar sum in bins of charged-particle
             multiplicity. These observables are unfolded to the
             stable-particle level, thereby correcting for migration
             effects due to finite detector resolution, acceptance and
             efficiency effects. The particle-level measurements are
             compared with different colour reconnection models in Monte
             Carlo generators. These measurements disfavour some of the
             colour reconnection models and provide inputs to future
             optimisation of the parameters in Monte Carlo
             generators.},
   Doi = {10.1140/epjc/s10052-023-11479-x},
   Key = {fds374029}
}

@article{fds359028,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Pereira, RA},
   Title = {Measurements of sensor radiation damage in the ATLAS inner
             detector using leakage currents},
   Journal = {Journal of Instrumentation},
   Volume = {16},
   Number = {8},
   Year = {2021},
   Month = {August},
   url = {http://dx.doi.org/10.1088/1748-0221/16/08/P08025},
   Abstract = {Non-ionizing energy loss causes bulk damage to the silicon
             sensors of the ATLAS pixel and strip detectors. This damage
             has important implications for data-taking operations,
             charged-particle track reconstruction, detector simulations,
             and physics analysis. This paper presents simulations and
             measurements of the leakage current in the ATLAS pixel
             detector and semiconductor tracker as a function of location
             in the detector and time, using data collected in Run 1
             (2010–2012) and Run 2 (2015–2018) of the Large Hadron
             Collider. The extracted fluence shows a much stronger
             |z|-dependence in the innermost layers than is seen in
             simulation. Furthermore, the overall fluence on the second
             innermost layer is significantly higher than in simulation,
             with better agreement in layers at higher radii. These
             measurements are important for validating the simulation
             models and can be used in part to justify safety factors for
             future detector designs and interventions.},
   Doi = {10.1088/1748-0221/16/08/P08025},
   Key = {fds359028}
}

@article{fds310339,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurements of spin correlation in top-antitop quark events
             from proton-proton collisions at √s =7 TeV using the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.112016},
   Abstract = {Measurements of spin correlation in top quark pair
             production are presented using data collected with the ATLAS
             detector at the LHC with proton-proton collisions at a
             center-of-mass energy of 7 TeV, corresponding to an
             integrated luminosity of 4.6 fb-1. Events are selected in
             final states with two charged leptons and at least two jets
             and in final states with one charged lepton and at least
             four jets. Four different observables sensitive to different
             properties of the top quark pair production mechanism are
             used to extract the correlation between the top and antitop
             quark spins. Some of these observables are measured for the
             first time. The measurements are in good agreement with the
             Standard Model prediction at next-to-leading-order
             accuracy.},
   Doi = {10.1103/PhysRevD.90.112016},
   Key = {fds310339}
}

@article{fds307814,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De
             Cecco, S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier,
             L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
             R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
             S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis,
             E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu,
             T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck,
             J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak,
             R and Maeshima, K and Makhoul, K and Maksimovic, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez,
             T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Santi,
             L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt,
             M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki,
             M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
             P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner,
             RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters,
             D and Weinberger, M and Wenzel, H and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T},
   Title = {Measurements of the angular distributions in the decays
             B→K(*)μ(+)μ(-) at CDF.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {8},
   Pages = {081807},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.108.081807},
   Abstract = {We report an indirect search for nonstandard model physics
             using the flavor-changing neutral current decays
             B→K(*)μ(+)μ(-). We reconstruct the decays and measure
             their angular distributions, as a function of
             q(2)=M(μμ)(2)c(2), where M(μμ) is the dimuon mass, in
             pp¯ collisions at √s=1.96 TeV using a data sample
             corresponding to an integrated luminosity of 6.8 fb(-1). The
             transverse polarization asymmetry A(T)(2) and the
             time-reversal-odd charge-and-parity asymmetry A(im) are
             measured for the first time, together with the K*
             longitudinal polarization fraction F(L) and the muon
             forward-backward asymmetry A(FB) for the decays
             B(0)→K(*0)μ(+)μ(-) and B(+)→K(*+)μ(+)μ(-). The
             B→K*μ(+)μ(-) forward-backward asymmetry in the most
             sensitive kinematic regime, 1≤q(2)<6 GeV(2)/c(2), is
             measured to be A(FB)=0.29(-0.23)(+0.20)(stat)±0.07(syst),
             the most precise result to date. No deviations from the
             standard model predictions are observed.},
   Doi = {10.1103/physrevlett.108.081807},
   Key = {fds307814}
}

@article{fds307710,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Measurements of the angular distributions of muons from Υ
             decays in pp collisions at sqrt[s] = 1.96  TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {15},
   Pages = {151802},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.108.151802},
   Abstract = {The angular distributions of muons from Υ(1S,2S,3S) → μ+
             μ- decays are measured using data from pp collisions at
             sqrt[s] = 1.96  TeV corresponding to an integrated
             luminosity of 6.7  fb(-1) and collected with the CDF II
             detector at the Fermilab Tevatron. This analysis is the
             first to report the full angular distributions as functions
             of transverse momentum p(T) for Υ mesons in both the
             Collins-Soper and s-channel helicity frames. This is also
             the first measurement of the spin alignment of Υ(3S)
             mesons. Within the kinematic range of Υ rapidity |y|<0.6
             and p(T) up to 40  GeV/c, the angular distributions are
             found to be nearly isotropic.},
   Doi = {10.1103/physrevlett.108.151802},
   Key = {fds307710}
}

@article{fds321109,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
   Title = {Measurements of the charge asymmetry in top-quark pair
             production in the dilepton final state at s =8 TeV with the
             ATLAS detector},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.032006},
   Abstract = {Measurements of the top-antitop quark pair production charge
             asymmetry in the dilepton channel, characterized by two
             high-pT leptons (electrons or muons), are presented using
             data corresponding to an integrated luminosity of 20.3 fb-1
             from pp collisions at a center-of-mass energy s=8 TeV
             collected with the ATLAS detector at the Large Hadron
             Collider at CERN. Inclusive and differential measurements as
             a function of the invariant mass, transverse momentum, and
             longitudinal boost of the tt system are performed both in
             the full phase space and in a fiducial phase space closely
             matching the detector acceptance. Two observables are
             studied: ACℓℓ based on the selected leptons and ACtt
             based on the reconstructed tt final state. The inclusive
             asymmetries are measured in the full phase space to be
             ACℓℓ=0.008±0.006 and ACtt=0.021±0.016, which are in
             agreement with the Standard Model predictions of
             ACℓℓ=0.0064±0.0003 and ACtt=0.0111±0.0004.},
   Doi = {10.1103/PhysRevD.94.032006},
   Key = {fds321109}
}

@article{fds307763,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Measurements of the electron and muon inclusive
             cross-sections in proton-proton collisions at √s=7TeV with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {707},
   Number = {5},
   Pages = {438-458},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.12.054},
   Abstract = {This Letter presents measurements of the differential
             cross-sections for inclusive electron and muon production in
             proton-proton collisions at a centre-of-mass energy of
             s=7TeV, using data collected by the ATLAS detector at the
             LHC. The muon cross-section is measured as a function of pT
             in the range 4<pT<100GeV and within pseudorapidity |η|<2.5.
             In addition the electron and muon cross-sections are
             measured in the range 7<pT<26GeV and within |η|<2.0,
             excluding 1.37<|η|<1.52. Integrated luminosities of 1.3pb-1
             and 1.4pb-1 are used for the electron and muon measurements,
             respectively. After subtraction of the W/Z/γ* contribution,
             the differential cross-sections are found to be in good
             agreement with theoretical predictions for heavy-flavour
             production obtained from Fixed Order NLO calculations with
             NLL high-pT resummation, and to be sensitive to the effects
             of NLL resummation. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.12.054},
   Key = {fds307763}
}

@article{fds352788,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
             MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
             CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA and Arcangeletti,
             C},
   Title = {Measurements of the Higgs boson inclusive and differential
             fiducial cross sections in the 4 ℓ decay channel at √s =
             13 TeV},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {10},
   Year = {2020},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-8223-0},
   Abstract = {Inclusive and differential fiducial cross sections of the
             Higgs boson are measured in the H→ ZZ∗→ 4 ℓ (ℓ= e,
             μ) decay channel. The results are based on proton−proton
             collision data produced at the Large Hadron Collider at a
             centre-of-mass energy of 13 TeV and recorded by the ATLAS
             detector from 2015 to 2018, equivalent to an integrated
             luminosity of 139 fb - 1. The inclusive fiducial cross
             section for the H→ ZZ∗→ 4 ℓ process is measured to
             be σfid= 3.28 ± 0.32 fb, in agreement with the Standard
             Model prediction of σfid , SM= 3.41 ± 0.18 fb.
             Differential fiducial cross sections are measured for a
             variety of observables which are sensitive to the production
             and decay of the Higgs boson. All measurements are in
             agreement with the Standard Model predictions. The results
             are used to constrain anomalous Higgs boson interactions
             with Standard Model particles.},
   Doi = {10.1140/epjc/s10052-020-8223-0},
   Key = {fds352788}
}

@article{fds321108,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Measurements of the Higgs boson production and decay rates
             and constraints on its couplings from a combined ATLAS and
             CMS analysis of the LHC pp collision data at √s = 7 and 8
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2016)045},
   Abstract = {Combined ATLAS and CMS measurements of the Higgs boson
             production and decay rates, as well as constraints on its
             couplings to vector bosons and fermions, are presented. The
             combination is based on the analysis of five production
             processes, namely gluon fusion, vector boson fusion, and
             associated production with a W or a Z boson or a pair of top
             quarks, and of the six decay modes H → ZZ, W W, γγ,
             ττ, bb, and μμ. All results are reported assuming a
             value of 125.09 GeV for the Higgs boson mass, the result of
             the combined measurement by the ATLAS and CMS experiments.
             The analysis uses the CERN LHC proton-proton collision data
             recorded by the ATLAS and CMS experiments in 2011 and 2012,
             corresponding to integrated luminosities per experiment of
             approximately 5 fb−1 at √s = 7 TeV and 20 fb−1 at √s
             = 8 TeV. The Higgs boson production and decay rates measured
             by the two experiments are combined within the context of
             three generic parameterisations: two based on cross sections
             and branching fractions, and one on ratios of coupling
             modifiers. Several interpretations of the measurements with
             more model-dependent parameterisations are also given. The
             combined signal yield relative to the Standard Model
             prediction is measured to be 1.09 ± 0.11. The combined
             measurements lead to observed significances for the vector
             boson fusion production process and for the H → ττ decay
             of 5.4 and 5.5 standard deviations, respectively. The data
             are consistent with the Standard Model predictions for all
             parameterisations considered.},
   Doi = {10.1007/JHEP08(2016)045},
   Key = {fds321108}
}

@article{fds346163,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
             P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
             S},
   Title = {Measurements of the Higgs boson production and decay rates
             and coupling strengths using pp collision data at
             [Formula: see text] and 8 TeV in the ATLAS
             experiment.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {6},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3769-y},
   Abstract = {Combined analyses of the Higgs boson production and decay
             rates as well as its coupling strengths to vector bosons and
             fermions are presented. The combinations include the results
             of the analyses of the [Formula: see text] and [Formula: see
             text] decay modes, and the constraints on the associated
             production with a pair of top quarks and on the off-shell
             coupling strengths of the Higgs boson. The results are based
             on the LHC proton-proton collision datasets, with integrated
             luminosities of up to 4.7 [Formula: see text] at [Formula:
             see text] TeV and 20.3 [Formula: see text] at [Formula: see
             text] TeV, recorded by the ATLAS detector in 2011 and 2012.
             Combining all production modes and decay channels, the
             measured signal yield, normalised to the Standard Model
             expectation, is [Formula: see text]. The observed Higgs
             boson production and decay rates are interpreted in a
             leading-order coupling framework, exploring a wide range of
             benchmark coupling models both with and without assumptions
             on the Higgs boson width and on the Standard Model particle
             content in loop processes. The data are found to be
             compatible with the Standard Model expectations for a Higgs
             boson at a mass of 125.36 GeV for all models
             considered.},
   Doi = {10.1140/epjc/s10052-015-3769-y},
   Key = {fds346163}
}

@article{fds359003,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
             M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
   Title = {Measurements of the inclusive and differential production
             cross sections of a top-quark–antiquark pair in
             association with a Z boson at √s=13 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {8},
   Year = {2021},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09439-4},
   Abstract = {Measurements of both the inclusive and differential
             production cross sections of a top-quark–antiquark pair in
             association with a Z boson (tt¯ Z) are presented. The
             measurements are performed by targeting final states with
             three or four isolated leptons (electrons or muons) and are
             based on s=13 TeV proton–proton collision data with an
             integrated luminosity of 139 fb - 1, recorded from 2015 to
             2018 with the ATLAS detector at the CERN Large Hadron
             Collider. The inclusive cross section is measured to be
             σtt¯Z= 0.99 ± 0.05 (stat.) ±0.08 (syst.) pb, in
             agreement with the most precise theoretical predictions. The
             differential measurements are presented as a function of a
             number of kinematic variables which probe the kinematics of
             the tt¯ Z system. Both absolute and normalised differential
             cross-section measurements are performed at particle and
             parton levels for specific fiducial volumes and are compared
             with theoretical predictions at different levels of
             precision, based on a χ2/ ndf and p value computation.
             Overall, good agreement is observed between the unfolded
             data and the predictions.},
   Doi = {10.1140/epjc/s10052-021-09439-4},
   Key = {fds359003}
}

@article{fds310303,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
   Title = {Measurements of the Nuclear Modification Factor for Jets in
             Pb+Pb Collisions at √(s)NN]=2.76  TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {7},
   Pages = {072302},
   Year = {2015},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.114.072302},
   Abstract = {Measurements of inclusive jet production are performed in pp
             and Pb+Pb collisions at √(s)NN=2.76  TeV with the
             ATLAS detector at the LHC, corresponding to integrated
             luminosities of 4.0 and 0.14  nb(-1), respectively. The
             jets are identified with the anti-k(t) algorithm with R=0.4,
             and the spectra are measured over the kinematic range of jet
             transverse momentum 32<p(T)<500  GeV and absolute
             rapidity |y|<2.1 and as a function of collision centrality.
             The nuclear modification factor R(AA) is evaluated, and jets
             are found to be suppressed by approximately a factor of 2 in
             central collisions compared to pp collisions. The R(AA)
             shows a slight increase with p(T) and no significant
             variation with rapidity.},
   Doi = {10.1103/physrevlett.114.072302},
   Key = {fds310303}
}

@article{fds347504,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
             A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti,
             M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
             J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez
             Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
             S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke,
             RN},
   Title = {Measurements of the production cross section of a [Formula:
             see text] boson in association with jets in pp
             collisions at [Formula: see text] TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {6},
   Pages = {361},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4900-z},
   Abstract = {Measurements of the production cross section of a [Formula:
             see text] boson in association with jets in proton-proton
             collisions at [Formula: see text] TeV are presented, using
             data corresponding to an integrated luminosity of
             3.16 fb[Formula: see text] collected by the ATLAS
             experiment at the CERN Large Hadron Collider in 2015.
             Inclusive and differential cross sections are measured for
             events containing a [Formula: see text] boson decaying to
             electrons or muons and produced in association with up to
             seven jets with [Formula: see text] GeV and [Formula: see
             text]. Predictions from different Monte Carlo generators
             based on leading-order and next-to-leading-order matrix
             elements for up to two additional partons interfaced with
             parton shower and fixed-order predictions at next-to-leading
             order and next-to-next-to-leading order are compared with
             the measured cross sections. Good agreement within the
             uncertainties is observed for most of the modelled
             quantities, in particular with the generators which use
             next-to-leading-order matrix elements and the more recent
             next-to-next-to-leading-order fixed-order
             predictions.},
   Doi = {10.1140/epjc/s10052-017-4900-z},
   Key = {fds347504}
}

@article{fds351088,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei,
             V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {Measurements of the production cross-section for a Z boson
             in association with b-jets in proton-proton collisions at
             √s = 13 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {7},
   Year = {2020},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2020)044},
   Abstract = {This paper presents a measurement of the production
             cross-section of a Z boson in association with b-jets, in
             proton-proton collisions at s = 13 TeV with the ATLAS
             experiment at the Large Hadron Collider using data
             corresponding to an integrated luminosity of 35.6 fb−1.
             Inclusive and differential cross-sections are measured for
             events containing a Z boson decaying into electrons or muons
             and produced in association with at least one or at least
             two b-jets with transverse momentum pT> 20 GeV and rapidity
             |y| < 2.5. Predictions from several Monte Carlo generators
             based on leading-order (LO) or next-to-leading-order (NLO)
             matrix elements interfaced with a parton-shower simulation
             and testing different flavour schemes for the choice of
             initial-state partons are compared with measured
             cross-sections. The 5-flavour number scheme predictions at
             NLO accuracy agree better with data than 4-flavour number
             scheme ones. The 4-flavour number scheme predictions
             underestimate data in events with at least one b-jet.
             [Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP07(2020)044},
   Key = {fds351088}
}

@article{fds313576,
   Author = {Aaltonen, T and González, BÃ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'Orso, M and Deluca,
             C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico,
             M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati,
             S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
             JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
             MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
             MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
             E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and Denis,
             RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
             J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel,
             M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester,
             WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang,
             YC},
   Title = {Measurements of the properties of Λc(2595),
             Λc(2625), Σc(2455), and Σ
             c(2520) baryons},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {84},
   Number = {1},
   Year = {2011},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.012003},
   Abstract = {We report measurements of the resonance properties of Λ
             c(2595)+ and Λc(2625)+ baryons in their decays to
             Λc+π+π- as well as Σc(2455)++,0 and Σ c(2520)++,0
             baryons in their decays to Λc+π± final states. These
             measurements are performed using data corresponding to
             5.2fb-1 of integrated luminosity from pp̄ collisions at
             √s=1.96TeV, collected with the CDF II detector at the
             Fermilab Tevatron. Exploiting the largest available charmed
             baryon sample, we measure masses and decay widths with
             uncertainties comparable to the world averages for Σc
             states, and significantly smaller uncertainties than the
             world averages for excited Λc+ states. © 2011 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.84.012003},
   Key = {fds313576}
}

@article{fds307674,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Measurements of the pseudorapidity dependence of the total
             transverse energy in proton-proton collisions at √s = 7TeV
             with ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {11},
   Pages = {1-53},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP11(2012)033},
   Abstract = {This paper describes measurements of the sum of the
             transverse energy of particles as a function of particle
             pseudorapidity, η, in proton-proton collisions at a
             centre-of-mass energy, √s = 7TeV using the ATLAS detector
             at the Large Hadron Collider. The measurements are performed
             in the region |η| < 4.8 for two event classes: those
             requiring the presence of particles with a low transverse
             momentum and those requiring particles with a significant
             transverse momentum. In the second dataset measurements are
             made in the region transverse to the hard scatter. The
             distributions are compared to the predictions of various
             Monte Carlo event generators, which generally tend to
             underestimate the amount of transverse energy at high |η|.
             Copyright CERN.},
   Doi = {10.1007/JHEP11(2012)033},
   Key = {fds307674}
}

@article{fds372218,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V},
   Title = {Measurements of the suppression and correlations of dijets
             in Pb+Pb collisions atsNN = 5.02
             TeV},
   Journal = {Physical Review C},
   Volume = {107},
   Number = {5},
   Year = {2023},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevC.107.054908},
   Abstract = {Studies of the correlations of the two highest transverse
             momentum (leading) jets in individual Pb+Pb collision events
             can provide information about the mechanism of jet quenching
             by the hot and dense matter created in such collisions. In
             Pb+Pb and pp collisions at√sNN = 5.02 TeV, measurements of
             the leading dijet transverse momentum (pT) correlations are
             presented. Additionally, measurements in Pb+Pb collisions of
             the dijet pair nuclear modification factors projected along
             leading and subleading jet pT are made. The measurements are
             performed using the ATLAS detector at the LHC with 260
             pb−1 of pp data collected in 2017 and 2.2 nb−1 of Pb+Pb
             data collected in 2015 and 2018. An unfolding procedure is
             applied to the two-dimensional leading and subleading jet pT
             distributions to account for experimental effects in the
             measurement of both jets. Results are provided for dijets
             with leading jet pT greater than 100 GeV. Measurements of
             the dijet-yield-normalized xJ distributions in Pb+Pb
             collisions show an increased fraction of imbalanced jets
             compared to pp collisions; these measurements are in
             agreement with previous measurements of the same quantity at
             2.76 TeV in the overlapping kinematic range. Measurements of
             the absolutely normalized dijet rate in Pb+Pb and pp
             collisions are also presented, and show that balanced dijets
             are significantly more suppressed than imbalanced dijets in
             Pb+Pb collisions. It is observed in the measurements of the
             pair nuclear modification factors that the subleading jets
             are significantly suppressed relative to leading jets with
             pT between 100 and 316 GeV for all centralities in Pb+Pb
             collisions.},
   Doi = {10.1103/PhysRevC.107.054908},
   Key = {fds372218}
}

@article{fds373464,
   Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Guillemin, T and Hryn'ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis,
             DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Sanchez
             Pineda, A and Sauvan, E and Selem, L and Bernardi, G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori, G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang, R and Zhang, J and Berlendis,
             S and Cheu, E and Cui, Z and Ghosh, A and Johns, KA and Lampl, W and Lindley,
             RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou,
             H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai,
             G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Tost, M and Unal, M and Huseynov, N},
   Title = {Measurements of the suppression and correlations of dijets
             in Xe+Xe collisions at Formula Presented
             TeV},
   Journal = {Physical Review C},
   Volume = {108},
   Number = {2},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevC.108.024906},
   Abstract = {Measurements of the suppression and correlations of dijets
             is performed using 3 µ b − 1 of Xe+Xe data at s N N =
             5.44 TeV collected with the ATLAS detector at the CERN Large
             Hadron Collider. Dijets with jets reconstructed using the R
             = 0.4 anti- k t algorithm are measured differentially in jet
             p T over the range of 32 to 398 GeV and the centrality of
             the collisions. Significant dijet momentum imbalance is
             found in the most central Xe+Xe collisions, which decreases
             in more peripheral collisions. Results from the measurement
             of per-pair normalized and absolutely normalized dijet p T
             balance are compared with previous Pb + Pb measurements at s
             N N = 5.02 TeV. The differences between the dijet
             suppression in Xe+Xe and Pb + Pb are further quantified by
             the ratio of pair nuclear-modification factors. The results
             are found to be consistent with those measured in Pb + Pb
             data when compared in classes of the same event activity and
             when taking into account the difference between the
             center-of-mass energies of the initial parton scattering
             process in Xe+Xe and Pb + Pb collisions. These results
             should provide input for a better understanding of the role
             of energy density, system size, path length, and
             fluctuations in the parton energy loss.},
   Doi = {10.1103/PhysRevC.108.024906},
   Key = {fds373464}
}

@article{fds313607,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurements of the top quark branching ratios into channels
             with leptons and quarks with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.072005},
   Abstract = {Measurements of the branching ratios of top quark decays
             into leptons and jets using events with tt (top antitop)
             pairs are reported. Events were recorded with the ATLAS
             detector at the LHC in pp collisions at a center-of-mass
             energy of 7 TeV. The collected data sample corresponds to an
             integrated luminosity of 4.6 fb-1. The measured top quark
             branching ratios agree with the Standard Model predictions
             within the measurement uncertainties of a few
             percent.},
   Doi = {10.1103/PhysRevD.92.072005},
   Key = {fds313607}
}

@article{fds307668,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Measurements of the top-quark mass and the tt cross section
             in the hadronic τ+jets decay channel at sqrt[s] = 1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {19},
   Pages = {192001},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.109.192001},
   Abstract = {We present the first direct measurement of the top-quark
             mass using tt events decaying in the hadronic τ+jets decay
             channel. Using data corresponding to an integrated
             luminosity of 2.2 fb(-1) collected by the CDF II detector in
             pp collisions at sqrt[s] = 1.96 TeV at the Fermilab
             Tevatron, we measure the tt cross section, σ(tt), and the
             top-quark mass, M(top). We extract M(top) from a likelihood
             based on per-event probabilities calculated with
             leading-order signal and background matrix elements. We
             measure σ(tt) = 8.8 ± 3.3(stat) ± 2.2(syst) pb and M(top)
             = 172.7 ± 9.3(stat) ± 3.7(syst) GeV/c(2).},
   Doi = {10.1103/physrevlett.109.192001},
   Key = {fds307668}
}

@article{fds307916,
   Author = {Aaltonen, and T, and others},
   Title = {Measurements of the top-quark mass using charged particle
             tracking},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {3},
   Pages = {032002},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.032002},
   Abstract = {http://arxiv.org/abs/0910.0969},
   Doi = {10.1103/PhysRevD.81.032002},
   Key = {fds307916}
}

@article{fds310262,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek,
             P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura,
             AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro,
             F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton,
             AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista,
             SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C and Conti, G},
   Title = {Measurements of the Total and Differential Higgs Boson
             Production Cross Sections Combining the H→γγ and
             H→ZZ^{*}→4ℓ Decay Channels at sqrt[s]=8  TeV with
             the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {115},
   Number = {9},
   Pages = {091801},
   Year = {2015},
   Month = {August},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.115.091801},
   Abstract = {Measurements of the total and differential cross sections of
             Higgs boson production are performed using 20.3  fb^{-1}
             of pp collisions produced by the Large Hadron Collider at a
             center-of-mass energy of sqrt[s]=8  TeV and recorded by
             the ATLAS detector. Cross sections are obtained from
             measured H→γγ and H→ZZ^{*}→4ℓ event yields, which
             are combined accounting for detector efficiencies, fiducial
             acceptances, and branching fractions. Differential cross
             sections are reported as a function of Higgs boson
             transverse momentum, Higgs boson rapidity, number of jets in
             the event, and transverse momentum of the leading jet. The
             total production cross section is determined to be
             σ_{pp→H}=33.0±5.3 (stat)±1.6 (syst)  pb. The
             measurements are compared to state-of-the-art
             predictions.},
   Doi = {10.1103/physrevlett.115.091801},
   Key = {fds310262}
}

@article{fds310317,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
             O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
             V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Measurements of the [Formula: see text] production cross
             sections in association with jets with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {2},
   Pages = {82},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3262-7},
   Abstract = {This paper presents cross sections for the production of a
             [Formula: see text] boson in association with jets, measured
             in proton-proton collisions at [Formula: see text] with the
             ATLAS experiment at the large hadron collider. With an
             integrated luminosity of [Formula: see text], this data set
             allows for an exploration of a large kinematic range,
             including jet production up to a transverse momentum of
             [Formula: see text] and multiplicities up to seven
             associated jets. The production cross sections for [Formula:
             see text] bosons are measured in both the electron and muon
             decay channels. Differential cross sections for many
             observables are also presented including measurements of the
             jet observables such as the rapidities and the transverse
             momenta as well as measurements of event observables such as
             the scalar sums of the transverse momenta of the jets. The
             measurements are compared to numerous QCD predictions
             including next-to-leading-order perturbative calculations,
             resummation calculations and Monte Carlo
             generators.},
   Doi = {10.1140/epjc/s10052-015-3262-7},
   Key = {fds310317}
}

@article{fds307648,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurements of top quark pair relative differential
             cross-sections with ATLAS in pp collisions at √s = 7
             TeV},
   Journal = {European Physical Journal C},
   Volume = {73},
   Number = {1},
   Pages = {1-28},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2261-1},
   Abstract = {Measurements are presented of differential crosss√ ections
             for top quark pair production in pp collisions at s = 7 TeV
             relative to the total inclusive top quark pair production
             cross-section. A data sample of 2.05 fb<sup>−1</sup>
             recorded by the ATLAS detector at the Large Hadron Collider
             is used. Relative differential cross-sections are derived as
             a function of the invariant mass, the transverse momentum
             and the rapidity of the top quark pair system. Events are
             selected in the lepton (electron or muon) + jets channel.
             The backgroundsubtracted differential distributions are
             corrected for detector effects, normalized to the total
             inclusive top quark pair production cross-section and
             compared to theoretical predictions. The measurement
             uncertainties range typically between 10 % and 20 % and are
             generally dominated by systematic effects. No significant
             deviations from the Standard Model expectations are
             observed.},
   Doi = {10.1140/epjc/s10052-012-2261-1},
   Key = {fds307648}
}

@article{fds356757,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
             H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
             D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurements of top quark spin observables in tt¯ events
             using dilepton final states in √s=8 TeV pp collisions with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {3},
   Year = {2017},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2017)113},
   Abstract = {Measurements of top quark spin observables in tt¯ events
             are presented based on 20.2 fb−1 of s=8 TeV proton-proton
             collisions recorded with the ATLAS detector at the LHC. The
             analysis is performed in the dilepton final state,
             characterised by the presence of two isolated leptons
             (electrons or muons). There are 15 observables, each
             sensitive to a different coefficient of the spin density
             matrix of tt¯ production, which are measured independently.
             Ten of these observables are measured for the first time.
             All of them are corrected for detector resolution and
             acceptance effects back to the parton and stable-particle
             levels. The measured values of the observables at parton
             level are compared to Standard Model predictions at
             next-to-leading order in QCD. The corrected distributions at
             stable-particle level are presented and the means of the
             distributions are compared to Monte Carlo predictions. No
             significant deviation from the Standard Model is observed
             for any observable.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP03(2017)113},
   Key = {fds356757}
}

@article{fds356558,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
             JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
             VA},
   Title = {Measurements of top-quark pair differential and
             double-differential cross-sections in the ℓ +jets channel
             with pp collisions at √s=13 TeV using the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {12},
   Year = {2019},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7525-6},
   Abstract = {Single- and double-differential cross-section measurements
             are presented for the production of top-quark pairs, in the
             lepton + jets channel at particle and parton level. Two
             topologies, resolved and boosted, are considered and the
             results are presented as a function of several kinematic
             variables characterising the top and tt¯ system and jet
             multiplicities. The study was performed using data from pp
             collisions at centre-of-mass energy of 13 TeV collected in
             2015 and 2016 by the ATLAS detector at the CERN Large Hadron
             Collider (LHC), corresponding to an integrated luminosity of
             36fb-1. Due to the large tt¯ cross-section at the LHC, such
             measurements allow a detailed study of the properties of
             top-quark production and decay, enabling precision tests of
             several Monte Carlo generators and fixed-order Standard
             Model predictions. Overall, there is good agreement between
             the theoretical predictions and the data.},
   Doi = {10.1140/epjc/s10052-019-7525-6},
   Key = {fds356558}
}

@article{fds321086,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho
             Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerny, K and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan,
             YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
   Title = {Measurements of top-quark pair differential cross-sections
             in the lepton+jets channel in pp collisions at
             [Formula: see text] using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {10},
   Pages = {538},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4366-4},
   Abstract = {Measurements of normalized differential cross-sections of
             top-quark pair production are presented as a function of
             the top-quark, [Formula: see text] system and event-level
             kinematic observables in proton-proton collisions at
             a centre-of-mass energy of [Formula: see text]. The
             observables have been chosen to emphasize the [Formula: see
             text] production process and to be sensitive to effects of
             initial- and final-state radiation, to the different parton
             distribution functions, and to non-resonant processes and
             higher-order corrections. The dataset corresponds to an
             integrated luminosity of 20.3 fb[Formula: see text],
             recorded in 2012 with the ATLAS detector at the CERN Large
             Hadron Collider. Events are selected in the lepton+jets
             channel, requiring exactly one charged lepton and at least
             four jets with at least two of the jets tagged as
             originating from a <i>b</i>-quark. The measured spectra are
             corrected for detector effects and are compared to several
             Monte Carlo simulations. The results are in fair agreement
             with the predictions over a wide kinematic range.
             Nevertheless, most generators predict a harder top-quark
             transverse momentum distribution at high values than what is
             observed in the data. Predictions beyond NLO accuracy
             improve the agreement with data at high top-quark transverse
             momenta. Using the current settings and parton distribution
             functions, the rapidity distributions are not well modelled
             by any generator under consideration. However, the level of
             agreement is improved when more recent sets of parton
             distribution functions are used.},
   Doi = {10.1140/epjc/s10052-016-4366-4},
   Key = {fds321086}
}

@article{fds356727,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Measurements of top-quark pair differential cross-sections
             in the lepton+jets channel in pp collisions at √s=13 TeV
             using the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {11},
   Year = {2017},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2017)191},
   Abstract = {Measurements of differential cross-sections of top-quark
             pair production in fiducial phase-spaces are presented as a
             function of top-quark and tt¯ system kinematic observables
             in proton-proton collisions at a centre-of-mass energy of
             s=13 TeV. The data set corresponds to an integrated
             luminosity of 3.2 fb−1, recorded in 2015 with the ATLAS
             detector at the CERN Large Hadron Collider. Events with
             exactly one electron or muon and at least two jets in the
             final state are used for the measurement. Two separate
             selections are applied that each focus on different
             top-quark momentum regions, referred to as resolved and
             boosted topologies of the tt¯ final state. The measured
             spectra are corrected for detector effects and are compared
             to several Monte Carlo simulations by means of calculated
             χ2 and p-values.},
   Doi = {10.1007/JHEP11(2017)191},
   Key = {fds356727}
}

@article{fds347499,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
             A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
             K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
             J and Billoud, TRV and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
             J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau,
             CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL},
   Title = {Measurements of top-quark pair differential cross-sections
             in the [Formula: see text] channel in pp collisions
             at [Formula: see text] TeV using the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {5},
   Pages = {292},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4821-x},
   Abstract = {This article presents measurements of [Formula: see text]
             differential cross-sections in a fiducial phase-space
             region, using an integrated luminosity of 3.2 fb[Formula:
             see text] of proton-proton data at a centre-of-mass energy
             of [Formula: see text] TeV recorded by the ATLAS experiment
             at the LHC in 2015. Differential cross-sections are measured
             as a function of the transverse momentum and absolute
             rapidity of the top quark, and of the transverse momentum,
             absolute rapidity and invariant mass of the [Formula: see
             text] system. The [Formula: see text] events are selected by
             requiring one electron and one muon of opposite electric
             charge, and at least two jets, one of which must be tagged
             as containing a <i>b</i>-hadron. The measured differential
             cross-sections are compared to predictions of
             next-to-leading order generators matched to parton showers
             and the measurements are found to be consistent with all
             models within the experimental uncertainties with the
             exception of the Powheg-Box [Formula: see text] Herwig++
             predictions, which differ significantly from the data in
             both the transverse momentum of the top quark and the mass
             of the [Formula: see text] system.},
   Doi = {10.1140/epjc/s10052-017-4821-x},
   Key = {fds347499}
}

@article{fds352201,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud,
             AA and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai,
             X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
             AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Estevez, MA and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
             JAA and Bella, LA and Arabidze, G and Araque, JP},
   Title = {Measurements of top-quark pair spin correlations in the eμ
             channel at √s=13 TeV using pp collisions in the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {8},
   Year = {2020},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-8181-6},
   Abstract = {A measurement of observables sensitive to spin correlations
             in tt¯ production is presented, using 36.1 fb - 1 of pp
             collision data at s=13 TeV recorded with the ATLAS detector
             at the Large Hadron Collider. Differential cross-sections
             are measured in events with exactly one electron and one
             muon with opposite-sign electric charge as a function of the
             azimuthal opening angle and the absolute difference in
             pseudorapidity between the electron and muon candidates in
             the laboratory frame. The azimuthal opening angle is also
             measured as a function of the invariant mass of the tt¯
             system. The measured differential cross-sections are
             compared to predictions by several NLO Monte Carlo
             generators and fixed-order calculations. The observed degree
             of spin correlation is somewhat higher than predicted by the
             generators used. The data are consistent with the prediction
             of one of the fixed-order calculations at NLO, but agree
             less well with higher-order predictions. Using these
             leptonic observables, a search is performed for pair
             production of supersymmetric top squarks decaying into
             Standard Model top quarks and light neutralinos. Top squark
             masses between 170 and 230 GeV are largely excluded at the
             95% confidence level for kinematically allowed values of the
             neutralino mass.},
   Doi = {10.1140/epjc/s10052-020-8181-6},
   Key = {fds352201}
}

@article{fds356764,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos,
             S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez,
             O},
   Title = {Measurements of top-quark pair to Z-boson cross-section
             ratios at √s=13 , 8, 7 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {2},
   Year = {2017},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP02(2017)117},
   Abstract = {Ratios of top-quark pair to Z-boson cross sections measured
             from proton-proton collisions at the LHC centre-of-mass
             energies of s=13 TeV, 8 TeV, and 7 TeV are presented by the
             ATLAS Collaboration. Single ratios, at a given s for the two
             processes and at different s for each process, as well as
             double ratios of the two processes at different s, are
             evaluated. The ratios are constructed using previously
             published ATLAS measurements of the tt¯ and Z-boson
             production cross sections, corrected to a common phase space
             where required, and a new analysis of Z → ℓ+ℓ− where
             ℓ = e, μ at s=13 TeV performed with data collected in
             2015 with an integrated luminosity of 3.2 fb−1.
             Correlations of systematic uncertainties are taken into
             account when evaluating the uncertainties in the ratios. The
             correlation model is also used to evaluate the combined
             cross section of the Z → e+e− and the Z → μ+μ−
             channels for each s value. The results are compared to
             calculations performed at next-to-next-to-leading-order
             accuracy using recent sets of parton distribution functions.
             The data demonstrate significant power to constrain the
             gluon distribution function for the Bjorken-x values near
             0.1 and the light-quark sea for x < 0.02.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP02(2017)117},
   Key = {fds356764}
}

@article{fds356708,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada
             Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza,
             A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O},
   Title = {Measurements of tt¯ differential cross-sections of highly
             boosted top quarks decaying to all-hadronic final states in
             pp collisions at √s =13 TeV using the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {1},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.012003},
   Abstract = {Measurements are made of differential cross-sections of
             highly boosted pair-produced top quarks as a function of
             top-quark and tt. system kinematic observables using
             proton-proton collisions at a center-of-mass energy of s=13
             TeV. The data set corresponds to an integrated luminosity of
             36.1 fb-1, recorded in 2015 and 2016 with the ATLAS detector
             at the CERN Large Hadron Collider. Events with two
             large-radius jets in the final state, one with transverse
             momentum pT>500 GeV and a second with pT>350 GeV, are used
             for the measurement. The top-quark candidates are separated
             from the multijet background using jet substructure
             information and association with a b-tagged jet. The
             measured spectra are corrected for detector effects to a
             particle-level fiducial phase space and a parton-level
             limited phase space, and are compared to several Monte Carlo
             simulations by means of calculated χ2 values. The
             cross-section for tt. production in the fiducial phase-space
             region is 292±7(stat)±71(syst) fb, to be compared to the
             theoretical prediction of 384±36 fb.},
   Doi = {10.1103/PhysRevD.98.012003},
   Key = {fds356708}
}

@article{fds357238,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
             JF},
   Title = {Measurements of W + W + ≥ 1 jet
             production cross-sections in pp collisions at √s = 13 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {6},
   Year = {2021},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2021)003},
   Abstract = {Fiducial and differential cross-section measurements of
             W+W− production in association with at least one hadronic
             jet are presented. These measurements are sensitive to the
             properties of electroweak-boson self-interactions and
             provide a test of perturbative quantum chromodynamics and
             the electroweak theory. The analysis is performed using
             proton-proton collision data collected at s = 13 TeV with
             the ATLAS experiment, corresponding to an integrated
             luminosity of 139 fb−1. Events are selected with exactly
             one oppositely charged electron-muon pair and at least one
             hadronic jet with a transverse momentum of pT> 30 GeV and a
             pseudorapidity of |η| < 4.5. After subtracting the
             background contributions and correcting for detector
             effects, the jet-inclusive W+W−+ ≥ 1 jet fiducial
             cross-section and W+W−+ jets differential cross-sections
             with respect to several kinematic variables are measured.
             These measurements include leptonic quantities, such as the
             lepton transverse momenta and the transverse mass of the
             W+W− system, as well as jet-related observables such as
             the leading jet transverse momentum and the jet
             multiplicity. Limits on anomalous triple-gauge-boson
             couplings are obtained in a phase space where interference
             between the Standard Model amplitude and the anomalous
             amplitude is enhanced. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP06(2021)003},
   Key = {fds357238}
}

@article{fds356628,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {Measurements of W and Z boson production in pp collisions at
             √s=5.02 TeV with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {2},
   Year = {2019},
   Month = {February},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-6622-x},
   Abstract = {Measurements of fiducial integrated and differential cross
             sections for inclusive W+, W- and Z boson production are
             reported. They are based on 25.0±0.5pb-1 of pp collision
             data at s=5.02 TeV collected with the ATLAS detector at the
             CERN Large Hadron Collider. Electron and muon decay channels
             are analysed, and the combined W+, W- and Z integrated cross
             sections are found to be σW+=2266±9(stat)±29(syst)±43(lumi) pb,
             σW-=1401±7(stat)±18(syst)±27(lumi) pb, and
             σZ=374.5±3.4(stat)±3.6(syst)±7.0(lumi) pb, in good
             agreement with next-to-next-to-leading-order QCD
             cross-section calculations. These measurements serve as
             references for Pb+Pb interactions at the LHC at
             sNN=5.02 TeV.},
   Doi = {10.1140/epjc/s10052-019-6622-x},
   Key = {fds356628}
}

@article{fds374027,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
             Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
             Bella, L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
             JF},
   Title = {Measurements of W+W- production in
             decay topologies inspired by searches for electroweak
             supersymmetry},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {8},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11508-9},
   Abstract = {This paper presents a measurement of fiducial and
             differential cross-sections for W+W- production in
             proton–proton collisions at s=13 TeV with the ATLAS
             experiment at the Large Hadron Collider using a dataset
             corresponding to an integrated luminosity of 139 fb - 1 .
             Events with exactly one electron, one muon and no hadronic
             jets are studied. The fiducial region in which the
             measurements are performed is inspired by searches for the
             electroweak production of supersymmetric charginos decaying
             to two-lepton final states. The selected events have
             moderate values of missing transverse momentum and the
             ‘stransverse mass’ variable mT2 , which is widely used
             in searches for supersymmetry at the LHC. The ranges of
             these variables are chosen so that the acceptance is
             enhanced for direct W+W- production and suppressed for
             production via top quarks, which is treated as a background.
             The fiducial cross-section and particle-level differential
             cross-sections for six variables are measured and compared
             with two theoretical SM predictions from perturbative QCD
             calculations.},
   Doi = {10.1140/epjc/s10052-023-11508-9},
   Key = {fds374027}
}

@article{fds355439,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
             KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
   Title = {Measurements of WH and ZH production in the H→ bb¯ decay
             channel in pp collisions at 13Te with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {2},
   Year = {2021},
   Month = {February},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-08677-2},
   Abstract = {Measurements of the Standard Model Higgs boson decaying into
             a bb¯ pair and produced in association with a W or Z boson
             decaying into leptons, using proton–proton collision data
             collected between 2015 and 2018 by the ATLAS detector, are
             presented. The measurements use collisions produced by the
             Large Hadron Collider at a centre-of-mass energy of s=13Te,
             corresponding to an integrated luminosity of 139fb-1. The
             production of a Higgs boson in association with a W or Z
             boson is established with observed (expected) significances
             of 4.0 (4.1) and 5.3 (5.1) standard deviations,
             respectively. Cross-sections of associated production of a
             Higgs boson decaying into bottom quark pairs with an
             electroweak gauge boson, W or Z, decaying into leptons are
             measured as a function of the gauge boson transverse
             momentum in kinematic fiducial volumes. The cross-section
             measurements are all consistent with the Standard Model
             expectations, and the total uncertainties vary from 30% in
             the high gauge boson transverse momentum regions to 85% in
             the low regions. Limits are subsequently set on the
             parameters of an effective Lagrangian sensitive to
             modifications of the WH and ZH processes as well as the
             Higgs boson decay into bb¯.},
   Doi = {10.1140/epjc/s10052-020-08677-2},
   Key = {fds355439}
}

@article{fds316851,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A},
   Title = {Measurements of W±Z production cross sections in pp
             collisions at s =8 TeV with the ATLAS detector and limits on
             anomalous gauge boson self-couplings},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {93},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {May},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.092004},
   Abstract = {This paper presents measurements of W±Z production in pp
             collisions at a center-of-mass energy of 8 TeV. The gauge
             bosons are reconstructed using their leptonic decay modes
             into electrons and muons. The data were collected in 2012 by
             the ATLAS experiment at the Large Hadron Collider and
             correspond to an integrated luminosity of 20.3 fb-1. The
             measured inclusive cross section in the detector fiducial
             region is σW±Z→ ′ν=35.1±0.9(stat)±0.8(sys)±0.8(lumi)
             fb, for one leptonic decay channel. In comparison, the
             next-to-leading-order Standard Model expectation is
             30.0±2.1 fb. Cross sections for W+Z and W-Z production and
             their ratio are presented as well as differential cross
             sections for several kinematic observables. Limits on
             anomalous triple gauge boson couplings are derived from the
             transverse mass spectrum of the W±Z system. From the
             analysis of events with a W and a Z boson associated with
             two or more forward jets an upper limit at 95% confidence
             level on the W±Z scattering cross section of 0.63 fb, for
             each leptonic decay channel, is established, while the
             Standard Model prediction at next-to-leading order is
             0.13±0.01 fb. Limits on anomalous quartic gauge boson
             couplings are also extracted.},
   Doi = {10.1103/PhysRevD.93.092004},
   Key = {fds316851}
}

@article{fds307597,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Measurements of Wγ and Zγ production in pp collisions at
             √s=7 TeV with the ATLAS detector at the
             LHC},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.112003},
   Abstract = {The integrated and differential fiducial cross sections for
             the production of a W or Z boson in association with a
             high-energy photon are measured using pp collisions at
             √s=7 TeV. The analyses use a data sample with an
             integrated luminosity of 4.6 fb-1 collected by the ATLAS
             detector during the 2011 LHC data-taking period. Events are
             selected using leptonic decays of the W and Z bosons
             [W(eν,μν) and Z(e+e-, μ+μ-,νν¯)] with the
             requirement of an associated isolated photon. The data are
             used to test the electroweak sector of the Standard Model
             and search for evidence for new phenomena. The measurements
             are used to probe the anomalous WWγ, ZZγ, and Zγγ
             triple-gauge-boson couplings and to search for the
             production of vector resonances decaying to Zγ and Wγ. No
             deviations from Standard Model predictions are observed and
             limits are placed on anomalous triple-gauge-boson couplings
             and on the production of new vector meson
             resonances.},
   Doi = {10.1103/PhysRevD.87.112003},
   Key = {fds307597}
}

@article{fds317304,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
   Title = {Measurements of Zγ and Zγγ production in pp collisions at
             s =8 TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {June},
   ISSN = {2470-0010},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.112002},
   Abstract = {The production of Z bosons with one or two isolated
             high-energy photons is studied using pp collisions at s=8
             TeV. The analyses use a data sample with an integrated
             luminosity of 20.3 fb-1 collected by the ATLAS detector
             during the 2012 LHC data taking. The Zγ and Zγγ
             production cross sections are measured with leptonic (e+e-,
             μ+μ-, νν) decays of the Z boson, in extended fiducial
             regions defined in terms of the lepton and photon
             acceptance. They are then compared to cross-section
             predictions from the Standard Model, where the sources of
             the photons are radiation off initial-state quarks and
             radiative Z-boson decay to charged leptons, and from
             fragmentation of final-state quarks and gluons into photons.
             The yields of events with photon transverse energy ET>250
             GeV from +-γ events and with ET>400 GeV from ννγ events
             are used to search for anomalous triple gauge-boson
             couplings ZZγ and Zγγ. The yields of events with diphoton
             invariant mass mγγ>200 GeV from +-γγ events and with
             mγγ>300 GeV from ννγγ events are used to search for
             anomalous quartic gauge-boson couplings ZZγγ and Zγγγ.
             No deviations from Standard Model predictions are observed
             and limits are placed on parameters used to describe
             anomalous triple and quartic gauge-boson
             couplings.},
   Doi = {10.1103/PhysRevD.93.112002},
   Key = {fds317304}
}

@article{fds356767,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Measurements of ψ(2S) and X(3872) → J/ψπ +
             π  production in pp collisions at √s=8 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {1},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2017)117},
   Abstract = {Differential cross sections are presented for the prompt and
             non-prompt production of the hidden-charm states X(3872) and
             ψ(2S), in the decay mode J/ψπ+π−, measured using 11.4
             fb−1 of pp collisions at s=8 TeV by the ATLAS detector at
             the LHC. The ratio of cross-sections X(3872)/ψ(2S) is also
             given, separately for prompt and non-prompt components, as
             well as the non-prompt fractions of X(3872) and ψ(2S).
             Assuming independent single effective lifetimes for
             non-prompt X(3872) and ψ(2S) production gives
             RB=ℬ(B→X(3872)+any)ℬ(X(3872)→J/ψπ+π−)/ℬ(B→ψ(2S)+any)ℬ(ψ(2S)→J/ψπ+π−)=(3.95±0.32(stat)±0.08(sys))×10−2
             separating short- and long-lived contributions, assuming
             that the short-lived component is due to Bc decays, gives RB
             = (3.57 ± 0.33(stat) ± 0.11(sys)) × 10−2, with the
             fraction of non-prompt X(3872) produced via Bc decays for
             pT(X(3872)) > 10 GeV being (25 ± 13(stat) ± 2(sys) ±
             5(spin))%. The distributions of the dipion invariant mass in
             the X(3872) and ψ(2S) decays are also measured and compared
             to theoretical predictions.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP01(2017)117},
   Key = {fds356767}
}

@article{fds347536,
   Author = {Shega, JW and Sunkara, PD and Kotwal, A and Kern, DW and Henning, SL and McClintock, MK and Schumm, P and Waite, LJ and Dale,
             W},
   Title = {Measuring cognition: the Chicago Cognitive Function Measure
             in the National Social Life, Health and Aging Project, Wave
             2.},
   Journal = {The journals of gerontology. Series B, Psychological
             sciences and social sciences},
   Volume = {69 Suppl 2},
   Pages = {S166-S176},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1093/geronb/gbu106},
   Abstract = {<h4>Objectives</h4>To describe the development of a
             multidimensional test of cognition for the National Social
             life, Health and Aging Project (NSHAP), the Chicago
             Cognitive Function Measure (CCFM).<h4>Method</h4>CCFM
             development included 3 steps: (a) A pilot test of the
             Montreal Cognitive Assessment (MoCA) to create a standard
             protocol, choose specific items, reorder items, and improve
             clarity; (b) integration into a CAPI-based format; and (c)
             evaluation of the performance of the CCFM in the field. The
             CCFM was subsequently incorporated into NSHAP, Wave 2 (n =
             3,377).<h4>Results</h4>The pre-test (n = 120) mean age was
             71.35 (SD 8.40); 53% were female, 69% white, and 70% with
             college or greater education. The MoCA took an average of
             15.6min; the time for the CCFM was 12.0 min. CCFM scores
             (0-20) can be used as a continuous outcome or to adjust for
             cognition in a multivariable analysis. CCFM scores were
             highly correlated with MoCA scores (r = .973). Modeling
             projects MoCA scores from CCFM scores using the equation:
             MoCA = (1.14 × CCFM) + 6.83. In Wave 2, the overall
             weighted mean CCFM score was 13.9 (SE 0.13).<h4>Discussion</h4>A
             survey-based adaptation of the MoCA was successfully
             integrated into a nationally representative sample of older
             adults, NSHAP Wave 2.},
   Doi = {10.1093/geronb/gbu106},
   Key = {fds347536}
}

@article{fds355713,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling,
             J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith,
             L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten,
             K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis,
             C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji,
             S and Balasubramanian, R and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton,
             AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso,
             MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
             F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia
             Bylund, O and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhatta, S and Bhattacharya, DS and Bhattarai,
             P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann,
             D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman, M and Bisanz, T and Biswal, JP and Biswas,
             D and Bitadze, A and Bittrich, C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bogavac, D and Bogdanchikov,
             AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler,
             S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton,
             CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati,
             L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carratta,
             G and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli, F and Cerny,
             K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
             DG and Charman, TP and Chatterjee, M and Chau, CC and Che, S and Chekanov,
             S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen,
             Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias,
             TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, YS and Christopher, LD and Chu, MC},
   Title = {Medium-Induced Modification of Z-Tagged Charged Particle
             Yields in Pb+Pb Collisions at 5.02 TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {126},
   Number = {7},
   Pages = {072301},
   Year = {2021},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.126.072301},
   Abstract = {The yield of charged particles opposite to a Z boson with
             large transverse momentum (p_{T}) is measured in
             260  pb^{-1} of pp and 1.7  nb^{-1} of Pb+Pb
             collision data at 5.02 TeV per nucleon pair recorded with
             the ATLAS detector at the Large Hadron Collider. The Z boson
             tag is used to select hard-scattered partons with specific
             kinematics, and to observe how their showers are modified as
             they propagate through the quark-gluon plasma created in
             Pb+Pb collisions. Compared with pp collisions,
             charged-particle yields in Pb+Pb collisions show significant
             modifications as a function of charged-particle p_{T} in a
             way that depends on event centrality and Z boson p_{T}. The
             data are compared with a variety of theoretical calculations
             and provide new information about the medium-induced energy
             loss of partons in a p_{T} regime difficult to measure
             through other channels.},
   Doi = {10.1103/physrevlett.126.072301},
   Key = {fds355713}
}

@article{fds362043,
   Author = {Bauer, M and Neubert, M},
   Title = {Minimal Leptoquark Explanation for the R_{D^{(*)}}, R_{K},
             and (g-2)_{μ} Anomalies.},
   Journal = {Physical review letters},
   Volume = {116},
   Number = {14},
   Pages = {141802},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2016},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.116.141802},
   Abstract = {We show that by adding a single new scalar particle to the
             standard model, a TeV-scale leptoquark with the quantum
             numbers of a right-handed down quark, one can explain in a
             natural way three of the most striking anomalies of particle
             physics: the violation of lepton universality in B[over
             ¯]→K[over ¯]ℓ^{+}ℓ^{-} decays, the enhanced B[over
             ¯]→D^{(*)}τν[over ¯] decay rates, and the anomalous
             magnetic moment of the muon. Constraints from other
             precision measurements in the flavor sector can be satisfied
             without fine-tuning. Our model predicts enhanced B[over
             ¯]→K[over ¯]^{(*)}νν[over ¯] decay rates and a
             new-physics contribution to B_{s}-B[over ¯]_{s} mixing
             close to the current central fit value.},
   Doi = {10.1103/physrevlett.116.141802},
   Key = {fds362043}
}

@article{fds347552,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Arduh, FA},
   Title = {Modelling radiation damage to pixel sensors in the ATLAS
             detector},
   Journal = {Journal of Instrumentation},
   Volume = {14},
   Number = {6},
   Year = {2019},
   Month = {June},
   url = {http://dx.doi.org/10.1088/1748-0221/14/06/P06012},
   Abstract = {Silicon pixel detectors are at the core of the current and
             planned upgrade of the ATLAS experiment at the LHC. Given
             their close proximity to the interaction point, these
             detectors will be exposed to an unprecedented amount of
             radiation over their lifetime. The current pixel detector
             will receive damage from non-ionizing radiation in excess of
             1015 1 MeV neq/cm2, while the pixel detector designed for
             the high-luminosity LHC must cope with an order of magnitude
             larger fluence. This paper presents a digitization model
             incorporating effects of radiation damage to the pixel
             sensors. The model is described in detail and predictions
             for the charge collection efficiency and Lorentz angle are
             compared with collision data collected between 2015 and 2017
             (≤ 10 1 MeV neq/cm2).},
   Doi = {10.1088/1748-0221/14/06/P06012},
   Key = {fds347552}
}

@article{fds346220,
   Author = {Kothekar, V and Kotwal, A},
   Title = {Molecular mechanics simulation of the interaction of
             estrogen receptor with estrogen regulatory
             element.},
   Journal = {Indian journal of biochemistry & biophysics},
   Volume = {29},
   Number = {4},
   Pages = {322-329},
   Year = {1992},
   Month = {August},
   Abstract = {A model for the interaction of 31 amino acid fragment
             (protein) from DNA binding domain of human estrogen receptor
             (hER) with a five base pair DNA sequence 5'GGTCA 3' from
             estrogen regulatory element (ERE) has been obtained using a
             step-wise procedure based on structural data on model
             peptides, DNA binding domain of hER, steric constrains
             imposed by tetrahedral coordination of the Cys sulphurs with
             zinc ion and classical secondary structural elements.
             Structure of the protein as well as its complex with DNA is
             obtained by energy minimization followed by refinement by
             molecular mechanics. The complex is stabilized by H-bonds
             between Lys22, Lys26 and Arg27 with DNA bases G2, T3 and T6.
             Lys22 also made H-bond with the backbone of G2. The backbone
             of Cys18 H-bonded with N7 of G1. DNA was in distorted B form
             and showed evidence of protein-induced conformational
             changes.},
   Key = {fds346220}
}

@article{fds310372,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Monitoring and data quality assessment of the ATLAS liquid
             argon calorimeter},
   Journal = {Journal of Instrumentation},
   Volume = {9},
   Number = {7},
   Pages = {P07024-P07024},
   Publisher = {IOP Publishing},
   Year = {2014},
   Month = {July},
   url = {http://dx.doi.org/10.1088/1748-0221/9/07/P07024},
   Abstract = {The liquid argon calorimeter is a key component of the ATLAS
             detector installed at the CERN Large Hadron Collider. The
             primary purpose of this calorimeter is the measurement of
             electron and photon kinematic properties. It also provides a
             crucial input for measuring jets and missing transverse
             momentum. An advanced data monitoring procedure was designed
             to quickly identify issues that would affect detector
             performance and ensure that only the best quality data are
             used for physics analysis. This article presents the
             validation procedure developed during the 2011 and 2012 LHC
             data-taking periods, in which more than 98% of the
             proton-proton luminosity recorded by ATLAS at a
             centre-of-mass energy of 7-8 TeV had calorimeter data
             quality suitable for physics analysis. © CERN 2014 for the
             benefit of the ATLAS collaboration.},
   Doi = {10.1088/1748-0221/9/07/P07024},
   Key = {fds310372}
}

@article{fds347539,
   Author = {Nair, V and Sharma, A and Kotwal, J and Bhikshapathy, M and Mishra, DK and Das, S and Sharma, S and Kapoor, R and Singh, J and Nair, V and Uday, Y and Kotwal, A},
   Title = {Monitoring of response to therapy with imatinib mesylate in
             Chronic Myeloid Leukemia in chronic phase
             (CML-CP).},
   Journal = {Medical journal, Armed Forces India},
   Volume = {70},
   Number = {4},
   Pages = {315-320},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.mjafi.2014.07.005},
   Abstract = {<h4>Background</h4>The BCR-ABL tyrosine kinase is a well
             validated therapeutic target in Chronic Myeloid Leukemia
             (CML). Imatinib mesylate (IM), a tyrosine kinase inhibitor
             is highly effective in the treatment of chronic phase CML.
             BCR - ABL transcripts have been well established as a
             molecular marker to document response to therapy in CML.
             Periodic monitoring of this marker helps in evolving
             therapeutic strategies with IM and also in diagnosing early
             relapse. This study was undertaken to monitor therapeutic
             response to IM in CML in chronic phase (CML-CP) by assessing
             BCR-ABL by real time quantitative PCR (RQ-PCR) techniques
             and to determine the effectiveness of the Indian generic
             IM.<h4>Methods</h4>One hundred consecutive patients of CML
             in chronic phase (CML-CP) were treated with an Indian
             generic of IM. Eighty-five patients were evaluable at 12
             months of therapy. At entry, diagnosis of CML-CP was
             confirmed by FISH and RQ-PCR. Response to therapy was
             monitored by assessing BCR-ABL levels by RQ-PCR at 6 and 12
             months of therapy. Regular follow up of patients was done to
             evaluate the safety profile of IM used in these
             patients.<h4>Results</h4>Complete hematological response
             (CHR) rates at 3, 6, 9 and 12 months were 92%, 94%, 100% and
             100% respectively. The total molecular response at 12 months
             was 43.52% of which complete molecular response (CMR) was
             noted in 17.64% and major molecular response (MMR) was
             observed in 25.88%. A cumulative survival probability of 0.8
             was observed.<h4>Conclusion</h4>The Indian generic molecule
             of IM is effective in the treatment of CML-CP. The cost of
             Indian generic molecule is less than Rs. 10,000 per month
             there by making this affordable for large number of CML-CP
             patients in India.},
   Doi = {10.1016/j.mjafi.2014.07.005},
   Key = {fds347539}
}

@article{fds307619,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
             M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker,
             OK and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer,
             F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro,
             A},
   Title = {Multi-channel search for squarks and gluinos in [Formula:
             see text]pp collisions with the ATLAS detector at the
             LHC.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {3},
   Pages = {2362},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2362-5},
   Abstract = {A search for supersymmetric particles in final states with
             zero, one, and two leptons, with and without jets identified
             as originating from <i>b</i>-quarks, in 4.7 fb<sup>-1</sup>
             of [Formula: see text]<i>pp</i> collisions produced by the
             Large Hadron Collider and recorded by the ATLAS detector is
             presented. The search uses a set of variables carrying
             information on the event kinematics transverse and parallel
             to the beam line that are sensitive to several topologies
             expected in supersymmetry. Mutually exclusive final states
             are defined, allowing a combination of all channels to
             increase the search sensitivity. No deviation from the
             Standard Model expectation is observed. Upper limits at
             95 % confidence level on visible cross-sections for the
             production of new particles are extracted. Results are
             interpreted in the context of the constrained minimal
             supersymmetric extension to the Standard Model and in
             supersymmetry-inspired models with diverse,
             high-multiplicity final states.},
   Doi = {10.1140/epjc/s10052-013-2362-5},
   Key = {fds307619}
}

@article{fds358347,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
             M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
   Title = {Muon reconstruction and identification efficiency in ATLAS
             using the full Run 2 pp collision data set at √s=13
             TeV},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {7},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09233-2},
   Abstract = {This article documents the muon reconstruction and
             identification efficiency obtained by the ATLAS experiment
             for 139 fb - 1 of pp collision data at s=13 TeV collected
             between 2015 and 2018 during Run 2 of the LHC. The increased
             instantaneous luminosity delivered by the LHC over this
             period required a reoptimisation of the criteria for the
             identification of prompt muons. Improved and newly developed
             algorithms were deployed to preserve high muon
             identification efficiency with a low misidentification rate
             and good momentum resolution. The availability of large
             samples of Z→ μμ and J/ ψ→ μμ decays, and the
             minimisation of systematic uncertainties, allows the
             efficiencies of criteria for muon identification, primary
             vertex association, and isolation to be measured with an
             accuracy at the per-mille level in the bulk of the phase
             space, and up to the percent level in complex kinematic
             configurations. Excellent performance is achieved over a
             range of transverse momenta from 3 GeV to several hundred
             GeV, and across the full muon detector acceptance of | η| <
             2.7.},
   Doi = {10.1140/epjc/s10052-021-09233-2},
   Key = {fds358347}
}

@article{fds310384,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson,
             M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
             G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker,
             OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella,
             G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat,
             P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
             M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley,
             AG and Buda, SI and Budagov, IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiarella,
             V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
             RN},
   Title = {Muon reconstruction efficiency and momentum resolution of
             the ATLAS experiment in proton-proton collisions at
             [Formula: see text] TeV in 2010.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {9},
   Pages = {3034},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3034-9},
   Abstract = {This paper presents a study of the performance of the muon
             reconstruction in the analysis of proton-proton collisions
             at [Formula: see text] TeV at the LHC, recorded by the
             ATLAS detector in 2010. This performance is described in
             terms of reconstruction and isolation efficiencies and
             momentum resolutions for different classes of reconstructed
             muons. The results are obtained from an analysis of
             [Formula: see text] meson and [Formula: see text] boson
             decays to dimuons, reconstructed from a data sample
             corresponding to an integrated luminosity of 40 pb[Formula:
             see text]. The measured performance is compared to Monte
             Carlo predictions and deviations from the predicted
             performance are discussed.},
   Doi = {10.1140/epjc/s10052-014-3034-9},
   Key = {fds310384}
}

@article{fds316854,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
             MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister,
             I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
             JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
             I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
             E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez
             Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
             S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
   Title = {Muon reconstruction performance of the ATLAS detector in
             proton-proton collision data at [Formula: see
             text]=13 TeV.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {292},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4120-y},
   Abstract = {This article documents the performance of the ATLAS muon
             identification and reconstruction using the LHC dataset
             recorded at [Formula: see text] TeV in 2015. Using a large
             sample of [Formula: see text] and [Formula: see text] decays
             from 3.2 fb[Formula: see text] of <i>pp</i> collision data,
             measurements of the reconstruction efficiency, as well as of
             the momentum scale and resolution, are presented and
             compared to Monte Carlo simulations. The reconstruction
             efficiency is measured to be close to [Formula: see text]
             over most of the covered phase space ([Formula: see text]
             and [Formula: see text] GeV). The isolation efficiency
             varies between 93 and [Formula: see text] depending on the
             selection applied and on the momentum of the muon. Both
             efficiencies are well reproduced in simulation. In the
             central region of the detector, the momentum resolution is
             measured to be [Formula: see text] ([Formula: see text]) for
             muons from [Formula: see text] ([Formula: see text]) decays,
             and the momentum scale is known with an uncertainty of
             [Formula: see text]. In the region [Formula: see text], the
             [Formula: see text] resolution for muons from [Formula: see
             text] decays is [Formula: see text] while the precision of
             the momentum scale for low-[Formula: see text] muons from
             [Formula: see text] decays is about [Formula: see
             text].},
   Doi = {10.1140/epjc/s10052-016-4120-y},
   Key = {fds316854}
}

@article{fds374214,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel,
             A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed,
             WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh,
             B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez,
             MA and Fernandez, AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen,
             T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
             J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez,
             O and Arnold, H and Tame, ZPA and Artoni, G and Asada, H and Asai, K and Asai,
             S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi,
             S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
             PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakos, E and Gupta, DB and Balasubramanian, R and Baldin,
             EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas,
             WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits,
             M-S and Barklow, T and Baron, P and Moreno, DAB and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Navarro, LB and Barreiro, F and da
             Costa, JBG and Barron, U and Teixeira, MGB and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Hurrell, LTB and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
             K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
             L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Kuutmann, EB and Berger, N and Bergmann, B and Beringer, J and Bernardi,
             G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta,
             P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
             V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Sola, JDB and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
             R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and de Renstrom, PAB and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Bunka, AT and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr,
             JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Vazquez, CJB and Buzykaev, AR and Cabras, G and Urbán,
             SC and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea,
             G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti,
             M and Toro, RC and Camarda, S and Munoz, DC and Camarri, P and Camerlingo,
             MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Bret, MC and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
             JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron,
             S and Carquin, E and Carrá, S and Carratta, G and Argos, FC and Carter,
             JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Garcia, LC and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
             J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Moursli, RCE and Cheu, E and Cheung, K and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi,
             K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
             BM and Clark, A},
   Title = {New techniques for jet calibration with the ATLAS
             detector},
   Journal = {The European Physical Journal C},
   Volume = {83},
   Number = {8},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11837-9},
   Abstract = {<jats:title>Abstract</jats:title><jats:p>A determination of
             the jet energy scale is presented using proton–proton
             collision data with a centre-of-mass energy of
             <jats:inline-formula><jats:alternatives><jats:tex-math>$$\sqrt{s}=13$$</jats:tex-math>??
             <mml:mrow> <mml:msqrt> <mml:mi>s</mml:mi> </mml:msqrt>
             <mml:mo>=</mml:mo> <mml:mn>13</mml:mn> </mml:mrow>
             </mml:math></jats:alternatives></jats:inline-formula> TeV,
             corresponding to an integrated luminosity of 140
             fb<jats:inline-formula><jats:alternatives><jats:tex-math>$$^{-1}$$</jats:tex-math>??
             <mml:msup> <mml:mrow /> <mml:mrow> <mml:mo>-</mml:mo>
             <mml:mn>1</mml:mn> </mml:mrow> </mml:msup>
             </mml:math></jats:alternatives></jats:inline-formula>
             collected using the ATLAS detector at the LHC. Jets are
             reconstructed using the ATLAS particle-flow method that
             combines charged-particle tracks and topo-clusters formed
             from energy deposits in the calorimeter cells. The
             anti-<jats:inline-formula><jats:alternatives><jats:tex-math>$$k_\textrm{t}$$</jats:tex-math>??
             <mml:msub> <mml:mi>k</mml:mi> <mml:mtext>t</mml:mtext>
             </mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
             jet algorithm with radius parameter <jats:inline-formula><jats:alternatives><jats:tex-math>$$R=0.4$$</jats:tex-math>??
             <mml:mrow> <mml:mi>R</mml:mi> <mml:mo>=</mml:mo>
             <mml:mn>0.4</mml:mn> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula>
             is used to define the jet. Novel jet energy scale
             calibration strategies developed for the LHC Run 2 are
             reported that lay the foundation for the jet calibration in
             Run 3. Jets are calibrated with a series of simulation-based
             corrections, including state-of-the-art techniques in jet
             calibration such as machine learning methods and novel in
             situ calibrations to achieve better performance than the
             baseline calibration derived using up to 81
             fb<jats:inline-formula><jats:alternatives><jats:tex-math>$$^{-1}$$</jats:tex-math>??
             <mml:msup> <mml:mrow /> <mml:mrow> <mml:mo>-</mml:mo>
             <mml:mn>1</mml:mn> </mml:mrow> </mml:msup>
             </mml:math></jats:alternatives></jats:inline-formula> of Run
             2 data. The performance of these new techniques is then
             examined in the in situ measurements by exploiting the
             transverse momentum balance between a jet and a reference
             object. The <jats:italic>b</jats:italic>-quark jet energy
             scale using particle flow jets is measured for the first
             time with around 1% precision using <jats:inline-formula><jats:alternatives><jats:tex-math>$$\gamma
             $$</jats:tex-math>?? <mml:mi>γ</mml:mi>
             </mml:math></jats:alternatives></jats:inline-formula>+jet
             events.</jats:p>},
   Doi = {10.1140/epjc/s10052-023-11837-9},
   Key = {fds374214}
}

@article{fds310116,
   Author = {Hays, C and Kotwal, A and Stelzer-Chilton, O},
   Title = {New techniques in the search for Z' bosons and other neutral
             resonances},
   Journal = {Modern Physics Letters A},
   Volume = {24},
   Number = {30},
   Pages = {2387-2403},
   Year = {2009},
   Month = {September},
   url = {http://dx.doi.org/10.1142/S021773230903179X},
   Abstract = {The search for neutral resonances at the energy frontier has
             a long and illustrious history, resulting in multiple
             discoveries. The canonical search scans the reconstructed
             invariant mass distribution of identified fermion pairs. Two
             recent analyses from the CDF experiment at the Fermilab
             Tevatron have applied novel methods to resonance searches.
             One analysis uses simulated templates to fit the inverse
             mass distribution of muon pairs, a quantity with
             approximately constant resolution for momenta measured with
             a tracking detector. The other analysis measures the angular
             distribution of electron pairs as a function of dielectron
             mass, gaining sensitivity over a probe of the mass spectrum
             alone. After reviewing several models that predict new
             neutral resonances, we discuss these CDF analyses and
             potential future applications. © 2009 World Scientific
             Publishing Company.},
   Doi = {10.1142/S021773230903179X},
   Key = {fds310116}
}

@article{fds347530,
   Author = {Kotwal, A and Biswas, D and Kakati, B and Bahadur, H and Gupta,
             N},
   Title = {Non traumatic keratitis due to colletotrichum coccodes: a
             case report.},
   Journal = {Journal of clinical and diagnostic research :
             JCDR},
   Volume = {9},
   Number = {2},
   Pages = {DD01-DD02},
   Year = {2015},
   Month = {February},
   url = {http://dx.doi.org/10.7860/jcdr/2015/10843.5529},
   Abstract = {Colletotrichum species, a rare and emerging fungus is a
             well- known plant pathogen and an uncommon cause of human
             infection. It has been implicated as the etiological agent
             of cutaneous phaeohyphomycosis and keratitis, particularly
             following colonization of traumatized tissues or in
             immunocompromised patients. However, it has hardly ever been
             reported in the absence of such predisposing risk factors.
             Here, we report a case of keratitis with Colletotrichum
             coccodes occurring in a middle- aged, immunocompetent person
             without any history of trauma or co-morbidity. The isolate
             was sensitive to Amphotericin B and Voriconazole, and
             accordingly the patient was treated successfully with ocular
             administration of Amphotericin B.},
   Doi = {10.7860/jcdr/2015/10843.5529},
   Key = {fds347530}
}

@article{fds308262,
   Author = {Troutman, R and Kotwal, A},
   Title = {Non-linear source/drain effects in amorphous-silicon
             thin-film transistors},
   Journal = {IEEE Transactions on Electron Devices},
   Volume = {36},
   Number = {11 pt 1},
   Pages = {2624},
   Year = {1989},
   Month = {November},
   Abstract = {Summary form only given. The authors discuss the effect of
             space-charge-limited conduction through the a-Si layer on
             n-channel staggered TFT (thin-film transistor)
             current-voltage characteristics by introducing a new model
             that incorporates this effect. Current density through the
             a-Si film can be described by J = βφ4, where φ is the
             potential from the channel to the source (or drain) contact.
             Field-effect mobility in an a-Si TFT increases with gate
             voltage because a greater fraction of the gate-induced
             electrons is in extended tail states as the Fermi level
             approaches the conduction band edge. Current flow at the
             ends of the channel is roughly analogous to the transmission
             line effect in shallow MOSFET source/drain diffusions, but
             the effect in TFTs is highly nonlinear because of the
             space-charge-limited current behavior. Experimental
             current-voltage characteristics measured on a variety of
             staggered TFTs closely match the simulated curves over a
             wide range of terminal voltages. Differential
             channel-conductance measurements of a-Si TFTs at a fixed
             gate voltage reveal a peak at low drain voltage with a sharp
             drop on the lower side. This behavior cannot be explained by
             models using linear series impedance, but it is accurately
             duplicated by the new model.},
   Key = {fds308262}
}

@article{fds307678,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'errico, M},
   Title = {Novel inclusive search for the Higgs boson in the
             four-lepton final state at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {7},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.072012},
   Abstract = {An inclusive search for the standard model Higgs boson using
             the four-lepton final state in proton-antiproton collisions
             produced by the Tevatron at √s=1.96TeV is conducted. The
             data are recorded by the CDF II detector and correspond to
             an integrated luminosity of 9.7fb -1. Three distinct Higgs
             decay modes, namely ZZ, WW, and ττ, are simultaneously
             probed. Nine potential signal events are selected and found
             to be consistent with the background expectation. We set a
             95% credibility limit on the production cross section times
             the branching ratio and subsequent decay to the four-lepton
             final state for hypothetical Higgs boson masses between
             120GeV/c2 and 300GeV/c2. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.86.072012},
   Key = {fds307678}
}

@article{fds349182,
   Author = {Kotwal, AV},
   Title = {Novel methods of constraining the parton distribution
             function uncertainty in the measurement of the W -boson
             mass},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {3},
   Year = {2018},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.033008},
   Abstract = {The measurement of the mass of the W boson is one of the
             most precise and impactful measurements to test the standard
             model (SM). Following the discovery of the Higgs boson and
             the measurement of its mass, all SM parameters are
             sufficiently well known in order to make precise predictions
             for electroweak observables such as the W boson mass. These
             observables receive corrections in extensions of the SM.
             Experimentally, the dominant uncertainty in the W-boson mass
             measurement at hadron colliders arises due to parton
             distribution functions (PDFs). We present novel in situ
             methods of constraining the PDF variation and of reducing
             the PDF impact on the W-mass measurement uncertainty at
             hadron colliders. These methods can exploit the very
             high-statistics samples of W-boson candidate events at the
             LHC.},
   Doi = {10.1103/PhysRevD.98.033008},
   Key = {fds349182}
}

@booklet{Adams95b,
   Author = {Adams, MR and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Breidung, H and Busza, W and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dhawan, SK and Dietrich, FS and Dougherty,
             W and Dreyer, T and Eckardt, V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen,
             KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Hughes, VW and Jackson, HE and Jaffe, DE and Jancso, G and Jansen, DM and Jin, Z and Kaufman, S and Kennedy, RD and Kinney, ER and Kirk, T and Kobrak, HG and Kotwal, AV and Kunori, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin, JG and Nickerson, RB and O'Day, S and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou,
             V},
   Title = {Nuclear decay following deep inelastic scattering of 470 GeV
             muons.},
   Journal = {Physical review letters},
   Volume = {74},
   Number = {26},
   Pages = {5198-5201},
   Year = {1995},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.74.5198},
   Doi = {10.1103/physrevlett.74.5198},
   Key = {Adams95b}
}

@booklet{Adams98,
   Author = {M. R. Adams and S. Aid and P. L. Anthony and D. A. Averill and M. D. Baker and B. R. Baller and A. Banerjee and A. A.
             Bhatti and U. Bratzler and H. M. Braun and H. Breidung and W. Busza and T. J. Carroll and H. L. Clark and J. M. Conrad and R. Davisson an},
   Title = {Nuclear decay following deep inelastic scattering of 470GeV
             muons (vol 74, pg 5198, 1995)},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {9},
   Pages = {2020 -- 2021},
   Year = {1998},
   Month = {March},
   Key = {Adams98}
}

@article{fds308054,
   Author = {Aaltonen, and T, and others},
   Title = {Observation and mass measurement of the baryon
             $Xi_b^-$},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {5},
   Pages = {052002},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.99.052002},
   Abstract = {We report the observation and measurement of the mass of the
             bottom, strange baryon Xib- through the decay chain
             Xib--->J/psiXi-, where J/psi-->µ+µ-, Xi--->Lambdapi-, and
             Lambda-->ppi-. A signal is observed whose probability of
             arising from a background fluctuation is 6.6{\AA}~10-15, or
             7.7 Gaussian standard deviations. The Xib- mass is measured
             to be 5792.9$\pm$2.5(stat) $\pm$1.7(syst)
             MeV/c2.},
   Doi = {10.1103/physrevlett.99.052002},
   Key = {fds308054}
}

@article{fds355023,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith,
             L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten,
             K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis,
             C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji,
             S and Balasubramanian, R and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton,
             AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso,
             MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
             F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia
             Bylund, O and Besson, N and Bethke, S and Betti, A and Bevan, AJ and Beyer,
             J and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman,
             M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich,
             C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla,
             JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska,
             HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
             JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner,
             L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr,
             JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti,
             P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capua, M and Cardarelli,
             R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carratta, G and Carter, JWS and Carter,
             TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, YS and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Chytka, L and Cieri, D},
   Title = {Observation and Measurement of Forward Proton Scattering in
             Association with Lepton Pairs Produced via the Photon Fusion
             Mechanism at ATLAS.},
   Journal = {Physical review letters},
   Volume = {125},
   Number = {26},
   Pages = {261801},
   Year = {2020},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.125.261801},
   Abstract = {The observation of forward proton scattering in association
             with lepton pairs (e^{+}e^{-}+p or μ^{+}μ^{-}+p) produced
             via photon fusion is presented. The scattered proton is
             detected by the ATLAS Forward Proton spectrometer, while the
             leptons are reconstructed by the central ATLAS detector.
             Proton-proton collision data recorded in 2017 at a
             center-of-mass energy of sqrt[s]=13  TeV are analyzed,
             corresponding to an integrated luminosity of
             14.6  fb^{-1}. A total of 57 (123) candidates in the
             ee+p (μμ+p) final state are selected, allowing the
             background-only hypothesis to be rejected with a
             significance exceeding 5 standard deviations in each
             channel. Proton-tagging techniques are introduced for
             cross-section measurements in the fiducial detector
             acceptance, corresponding to σ_{ee+p}=11.0±2.6(stat)±1.2(syst)±0.3(lumi)
             and σ_{μμ+p}=7.2±1.6(stat)±0.9(syst)±0.2(lumi)  fb
             in the dielectron and dimuon channel, respectively.},
   Doi = {10.1103/physrevlett.125.261801},
   Key = {fds355023}
}

@article{fds310273,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Observation and measurement of Higgs boson decays to
             WWwith the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.012006},
   Abstract = {We report the observation of Higgs boson decays to
             WW∗based on an excess over background of 6.1 standard
             deviations in the dilepton final state, where the Standard
             Model expectation is 5.8 standard deviations. Evidence for
             the vector-boson fusion (VBF) production process is obtained
             with a significance of 3.2 standard deviations. The results
             are obtained from a data sample corresponding to an
             integrated luminosity of 25 fb-1from √s = 7 and 8 TeV pp
             collisions recorded by the ATLAS detector at the LHC. For a
             Higgs boson mass of 125.36 GeV, the ratio of the measured
             value to the expected value of the total production cross
             section times branching fraction is 1.09+0.16-0.15(stat)+0.17-0.14(syst).
             The corresponding ratios for the gluon fusion and
             vector-boson fusion production mechanisms are 1.02 ±
             0.19(stat)+0.22-0.18(syst) and 1.27+0.44-0.40(stat)+0.30-0.21(syst),
             respectively. At √s = 8 TeV, the total production cross
             sections are measured to be σ(gg→H→WW∗)=4.6±0.9(stat)+0.8-0.7(syst)
             pb and σ(VBF H → WW∗)=0.51+0.17-0.15(stat)+0.13-0.08(syst)pb.
             The fiducial cross section is determined for the
             gluon-fusion process in exclusive final states with zero or
             one associated jet.},
   Doi = {10.1103/PhysRevD.92.012006},
   Key = {fds310273}
}

@article{fds313601,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov,
             SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
             A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell,
             WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger,
             N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C and Conti, G and Conventi, F and Cooke, M and Cooper,
             BD},
   Title = {Observation and measurements of the production of prompt and
             non-prompt [Formula: see text] mesons in association with a
             [Formula: see text] boson in [Formula: see text] collisions
             at [Formula: see text] with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {5},
   Pages = {229},
   Year = {2015},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3406-9},
   Abstract = {The production of a [Formula: see text] boson in association
             with a [Formula: see text] meson in proton-proton collisions
             probes the production mechanisms of quarkonium and heavy
             flavour in association with vector bosons, and allows
             studies of multiple parton scattering. Using [Formula: see
             text] of data collected with the ATLAS experiment at the LHC
             in [Formula: see text] collisions at [Formula: see text],
             the first measurement of associated [Formula: see text]
             production is presented for both prompt and non-prompt
             [Formula: see text] production, with both signatures having
             a significance in excess of [Formula: see text]. The
             inclusive production cross-sections for [Formula: see text]
             boson production (analysed in [Formula: see text] or
             [Formula: see text] decay modes) in association with prompt
             and non-prompt [Formula: see text] are measured relative to
             the inclusive production rate of [Formula: see text] bosons
             in the same fiducial volume to be [Formula: see text] and
             [Formula: see text] respectively. Normalised differential
             production cross-section ratios are also determined as a
             function of the [Formula: see text] transverse momentum. The
             fraction of signal events arising from single and double
             parton scattering is estimated, and a lower limit of
             [Formula: see text] at [Formula: see text] confidence level
             is placed on the effective cross-section regulating double
             parton interactions.},
   Doi = {10.1140/epjc/s10052-015-3406-9},
   Key = {fds313601}
}

@article{fds308160,
   Author = {Abazov, VM and Abbott, B and Abolins, M and Acharya, BS and Adams, DL and Adams, M and Adams, T and Agelou, M and Agram, J-L and Ahmed, SN and Ahn,
             SH and Alexeev, GD and Alkhazov, G and Alton, A and Alverson, G and Alves,
             GA and Anderson, S and Andrieu, B and Arnoud, Y and Askew, A and Asman, B and Autermann, C and Avila, C and Babukhadia, L and Bacon, TC and Baden, A and Baffioni, S and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Bargassa, P and Baringer, P and Barnes, C and Barreto, J and Bartlett,
             JF and Bassler, U and Bauer, D and Bean, A and Beauceron, S and Beaudette,
             F and Begel, M and Beri, SB and Bernardi, G and Bertram, I and Besançon,
             M and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Binder, M and Bischoff, A and Black, KM and Blackler, I and Blazey, G and Blekman, F and Bloch, D and Blumenschein, U and Boehnlein, A and Bolton, TA and Bonamy, P and Borcherding, F and Borissov, G and Bos, K and Bose, T and Boswell, C and Brandt, A and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burdin, S and Burnett,
             TH and Busato, E and Butler, JM and Bystricky, J and Canelli, F and Carvalho, W and Casey, BCK and Casey, D and Cason, NM and Castilla-Valdez, H and Chakrabarti, S and Chakraborty, D and Chan,
             KM and Chandra, A and Chapin, D and Charles, F and Cheu, E and Chevalier,
             L and Cho, DK and Choi, S and Chopra, S and Christiansen, T and Christofek,
             L and Claes, D and Clark, AR and Clément, C and Coadou, Y and Colling, DJ and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Corcoran, M and Coss, J and Cothenet, A and Cousinou, M-C and Crépé-Renaudin, S and Cristetiu, M and Cummings, MAC and Cutts, D and da Motta, H and Davies,
             B and Davies, G and Davis, GA and De, K and de Jong, P and de Jong, SJ and De
             La Cruz-Burelo and E and De Oliveira Martins and C and Dean, S and Del
             Signore, K and Déliot, F and Delsart, PA and Demarteau, M and Demina,
             R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doidge, M and Dong, H and Doulas, S and Duflot, L and Dugad, SR and Duperrin, A and Dyer, J and Dyshkant, A and Eads, M and Edmunds, D and Edwards, T and Ellison, J and Elmsheuser, J and Eltzroth,
             JT and Elvira, VD and Eno, S and Ermolov, P and Eroshin, OV and Estrada, J and Evans, D and Evans, H and Evdokimov, A and Evdokimov, VN and Fast, J and Fatakia, SN and Fein, D and Feligioni, L and Ferbel, T and Fiedler, F and Filthaut, F and Fisk, HE and Fleuret, F and Fortner, M and Fox, H and Freeman, W and Fu, S and Fuess, S and Galea, CF and Gallas, E and Galyaev,
             E and Gao, M and Garcia, C and Garcia-Bellido, A and Gardner, J and Gavrilov, V and Gelé, D and Gelhaus, R and Genser, K and Gerber, CE and Gershtein, Y and Geurkov, G and Ginther, G and Goldmann, K and Golling,
             T and Gómez, B and Gounder, K and Goussiou, A and Graham, G and Grannis,
             PD and Greder, S and Green, JA and Greenlee, H and Greenwood, ZD and Gregores, EM and Grinstein, S and Grivaz, J-F and Groer, L and Grünendahl, S and Grünewald, MW and Gu, W and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Haas, A and Hadley, NJ and Haggerty,
             H and Hagopian, S and Hall, I and Hall, RE and Han, C and Han, L and Hanagaki,
             K and Hanlet, P and Harder, K and Hauptman, JM and Hauser, R and Hays, C and Hays, J and Hebert, C and Hedin, D and Heinmiller, JM and Heinson, AP and Heintz, U and Hensel, C and Hesketh, G and Hildreth, MD and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hohlfeld, M and Hong, SJ and Hooper, R and Hou, S and Hu, Y and Huang, J and Huang, Y and Iashvili, I and Illingworth,
             R and Ito, AS and Jabeen, S and Jaffré, M and Jain, S and Jain, V and Jakobs,
             K and Jenkins, A and Jesik, R and Jiang, Y and Johns, K and Johnson, M and Johnson, P and Jonckheere, A and Jonsson, P and Jöstlein, H and Juste,
             A and Kado, MM and Käfer, D and Kahl, W and Kahn, S and Kajfasz, E and Kalinin, AM and Kalk, J and Karmanov, D and Kasper, J and Kau, D and Ke, Z and Kehoe, R and Kermiche, S and Kesisoglou, S and Khanov, A and Kharchilava, A and Kharzheev, YM and Kim, KH and Klima, B and Klute, M and Kohli, JM and Kopal, M and Korablev, V and Kotcher, J and Kothari, B and Kotwal, AV and Koubarovsky, A and Kouchner, A and Kouznetsov, O and Kozelov, AV and Kozminski, J and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kurca, T and Kuznetsov, VE and Lager, S and Lahrichi, N and Landsberg, G and Lazoflores, J and Le Bihan and A-C and Lebrun, P and Lee, SW and Lee, WM and Leflat, A and Leggett, C and Lehner,
             F and Leonidopoulos, C and Lewis, P and Li, J and Li, QZ and Li, X and Lima,
             JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lobo, L and Lobodenko, A and Lokajicek, M and Lounis, A and Lu, J and Lubatti, HJ and Lucotte, A and Lueking, L and Luo, C and Lynker, M and Lyon, AL and Maciel,
             AKA and Madaras, RJ and Mättig, P and Magnan, A-M and Maity, M and Mal,
             PK and Malik, S and Malyshev, VL and Manankov, V and Mao, HS and Maravin,
             Y and Marshall, T and Martens, M and Martin, MI and Mattingly, SEK and Mayorov, AA and McCarthy, R and McCroskey, R and McMahon, T and Meder,
             D and Melanson, HL and Melnitchouk, A and Meng, X and Merkin, M and Merritt, KW and Meyer, A and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mitrevski, J and Mokhov, N and Molina, J and Mondal, NK and Montgomery, HE and Moore, RW and Mostafa, M and Muanza, GS and Mulders,
             M and Mutaf, YD and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Naumann, NA and Neal, HA and Negret, JP and Nelson, S and Neustroev, P and Noeding, C and Nomerotski, A and Novaes, SF and Nunnemann, T and Nurse,
             E and O'Dell, V and O'Neil, DC and Oguri, V and Oliveira, N and Olivier, B and Oshima, N and Otero y Garzón and GJ and Padley, P and Papageorgiou, K and Parashar, N and Park, J and Park, SK and Parsons, J and Partridge, R and Parua, N and Patwa, A and Perea, PM and Perez, E and Peters, O and Pétroff, P and Petteni, M and Phaf, L and Piegaia, R and Podesta-Lerma,
             PLM and Podstavkov, VM and Pope, BG and Popkov, E and Prado da Silva,
             WL and Prosper, HB and Protopopescu, S and Przybycien, MB and Qian, J and Quadt, A and Quinn, B and Rani, KJ and Rapidis, PA and Ratoff, PN and Reay,
             NW and Renardy, J-F and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Ripp-Baudot, I and Rizatdinova, F and Royon, C and Rubinov, P and Ruchti, R and Sabirov, BM and Sajot, G and Sánchez-Hernández, A and Sanders, MP and Santoro, A and Savage, G and Sawyer, L and Scanlon, T and Schamberger, RD and Schellman, H and Schieferdecker, P and Schmitt, C and Schukin, A and Schwartzman, A and Schwienhorst, R and Sengupta, S and Shabalina, E and Shary, V and Shephard, WD and Shpakov, D and Sidwell, RA and Simak, V and Sirotenko,
             V and Skow, D and Slattery, P and Smith, RP and Smolek, K and Snow, GR and Snow, J and Snyder, S and Söldner-Rembold, S and Song, X and Song, Y and Sonnenschein, L and Sopczak, A and Sorín, V and Sosebee, M and Soustruznik, K and Souza, M and Stanton, NR and Stark, J and Steele, J and Steinbrück, G and Stevenson, K and Stolin, V and Stone, A and Stoyanova, DA and Strandberg, J and Strang, MA and Strauss, M and Ströhmer, R and Strovink, M and Stutte, L and Sznajder, A and Talby, M and Tamburello, P and Taylor, W and Telford, P and Temple, J and Tentindo-Repond, S and Thomas, E and Thooris, B and Tomoto,
             M},
   Title = {Observation and properties of the X(3872) decaying to
             J/psipi(+)pi(-) in pp collisions at sqrt[s]=1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {93},
   Number = {16},
   Pages = {162002},
   Year = {2004},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.93.162002},
   Abstract = {We report the observation of the X(3872) in the
             J/psipi(+)pi(-) channel, with J/psi decaying to mu(+)mu(-),
             in pp collisions at sqrt[s]=1.96 TeV. Using approximately
             230 pb(-1) of data collected with the Run II D0 detector, we
             observe 522+/-100 X(3872) candidates. The mass difference
             between the X(3872) state and the J/psi is measured to be
             774.9+/-3.1(stat)+/-3.0(syst) MeV/c(2). We have investigated
             the production and decay characteristics of the X(3872) and
             find them to be similar to those of the psi(2S)
             state.},
   Doi = {10.1103/physrevlett.93.162002},
   Key = {fds308160}
}

@article{fds308085,
   Author = {Abulencia, and A, and others},
   Title = {Observation of $B^0_s \to K^{+} K^{-}$ and Measurements of
             Branching Fractions of Charmless Two-body Decays of $B^0$
             and $B^0_{s}$ Mesons in $\bar{p} p$ Collisions at $\sqrt{s}$
             = 1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {97},
   Number = {21},
   Pages = {211802},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.97.211802},
   Abstract = {We search for decays of the type B(s)0-->h+h[prime]- (where
             h,h[prime]=K or pi) in 180 pb-1 of [overline p]p collisions
             collected at the Tevatron by the upgraded Collider Detector
             at Fermilab. We report the first observation of the new mode
             Bs0-->K+K- with a yield of 236$\pm$32 events, corresponding
             to (fs/fd)?[script B](Bs0-->K+K-)/[script
             B](B0-->K+pi-)=0.46$\pm$0.08(stat)$\pm$0.07(syst), where
             fs/fd is the ratio of production fractions of Bs0 and B0. We
             find results in agreement with world averages for the B0
             modes, and set the following new limits at 90\% C.L.:
             [script B](Bs0-->K-pi+)s0-->pi+pi-)},
   Doi = {10.1103/physrevlett.97.211802},
   Key = {fds308085}
}

@article{fds308057,
   Author = {Abulencia, and A, and others},
   Title = {Observation of $WZ$ Production},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {16},
   Pages = {161801},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.161801},
   Abstract = {We report the first observation of the associated production
             of a W boson and a Z boson. This result is based on 1.1 fb-1
             of integrated luminosity from p[overline p] collisions at
             sqrt(s)=1.96 TeV collected with the CDF II detector at the
             Fermilab Tevatron. We observe 16 WZ candidates passing our
             event selection with an expected background of 2.7$\pm$0.4
             events. A fit to the missing transverse energy distribution
             indicates an excess of events compared to the background
             expectation corresponding to a significance equivalent to 6
             standard deviations. The measured cross section is
             sigma(p[overline p]-->WZ)=5.0-1.6+1.8 pb, consistent with
             the standard model expectation.},
   Doi = {10.1103/physrevlett.98.161801},
   Key = {fds308057}
}

@article{fds307876,
   Author = {Aaltonen, and T, and al, E},
   Title = {Observation of ${B}_{s}^{0}$\rightarrow${}J/$\psi${}{K}^{*}(892{)}^{0}$
             and ${B}_{s}^{0}$\rightarrow${}J/$\psi${}{K}_{S}^{0}$
             decays},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {5},
   Pages = {052012},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.052012},
   Abstract = {We report the first observation of two Cabibbo-suppressed
             decay modes of the Bs0 meson. Using a sample of pp̄
             collisions at √s=1.96TeV corresponding to 5.9fb-1 of
             integrated luminosity collected with the CDF II, the
             collider detector at the Fermilab Tevatron, we search for
             new Bs0 decay modes in a sample of events containing
             J/ψ→μ+μ - decays. We reconstruct a Bs0→J/ψK*(892)0
             signal with K*(892)0→K+π-, observing a yield of 151±25
             events with a statistical significance of 8.0σ. We also
             reconstruct a Bs0→J/ψKS0 signal with KS0→π+π-,
             observing a yield of 64±14 events with a statistical
             significance of 7.2σ. From these yields, we extract the
             branching ratios B(Bs0→J/ψK*(892)0)=(8. 3±3.8)×10-5 and
             B(Bs0→J/ψK0)=(3.5±0.8) ×10-5, where statistical,
             systematic, and fragmentation- fraction uncertainties are
             included in the combined uncertainty. © 2011 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.83.052012},
   Key = {fds307876}
}

@article{fds307719,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and A°kesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, JF and Arik, E},
   Title = {Observation of a new particle in the search for the Standard
             Model Higgs boson with the ATLAS detector at the
             LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {716},
   Number = {1},
   Pages = {1-29},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.08.020},
   Abstract = {A search for the Standard Model Higgs boson in proton-proton
             collisions with the ATLAS detector at the LHC is presented.
             The datasets used correspond to integrated luminosities of
             approximately 4.8 fb -1 collected at s=7 TeV in 2011 and 5.8
             fb -1 at s=8 TeV in 2012. Individual searches in the
             channels H→ZZ (*) →4ℓ, H→γγ and H→WW (*)
             →eνμν in the 8 TeV data are combined with previously
             published results of searches for H→ZZ (*) , WW (*) , bb-
             and τ + τ - in the 7 TeV data and results from improved
             analyses of the H→ZZ (*) →4ℓ and H→γγ channels in
             the 7 TeV data. Clear evidence for the production of a
             neutral boson with a measured mass of 126.0±0.4(stat)±0.4(sys)GeV
             is presented. This observation, which has a significance of
             5.9 standard deviations, corresponding to a background
             fluctuation probability of 1.7×10 -9 , is compatible with
             the production and decay of the Standard Model Higgs boson.
             © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.08.020},
   Key = {fds307719}
}

@article{fds307708,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Observation of a new χ(b) state in radiative transitions to
             Υ(1S) and Υ(2S) at ATLAS.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {15},
   Pages = {152001},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.108.152001},
   Abstract = {The χ(b)(nP) quarkonium states are produced in
             proton-proton collisions at the Large Hadron Collider at
             sqrt[s] = 7  TeV and recorded by the ATLAS detector.
             Using a data sample corresponding to an integrated
             luminosity of 4.4  fb(-1), these states are
             reconstructed through their radiative decays to Υ(1S,2S)
             with Υ → μ+ μ-. In addition to the mass peaks
             corresponding to the decay modes χ(b)(1P,2P) → Υ(1S)γ,
             a new structure centered at a mass of 10.530 ± 0.005(stat)
             ± 0.009(syst)  GeV is also observed, in both the
             Υ(1S)γ and Υ(2S)γ decay modes. This structure is
             interpreted as the χ(b)(3P) system.},
   Doi = {10.1103/physrevlett.108.152001},
   Key = {fds307708}
}

@article{fds373609,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
             J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
             Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
             GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
             M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
             JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
             C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
             KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
             J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez,
             O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol,
             AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal,
             D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour,
             G and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr,
             AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
             M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano
             Hurrell, LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
             F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov,
             VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
             M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir,
             M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal,
             J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
             R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
             PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
             CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo
             Vazquez, CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir,
             O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
             Bret, M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone,
             A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin,
             E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo,
             FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
             J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F},
   Title = {Observation of an Excess of Dicharmonium Events in the
             Four-Muon Final State with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {131},
   Number = {15},
   Pages = {151902},
   Year = {2023},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.131.151902},
   Abstract = {A search is made for potential ccc[over ¯]c[over ¯]
             tetraquarks decaying into a pair of charmonium states in the
             four muon final state using proton-proton collision data at
             sqrt[s]=13  TeV, corresponding to an integrated
             luminosity of 140  fb^{-1} recorded by the ATLAS
             experiment at LHC. Two decay channels, J/ψ+J/ψ→4μ and
             J/ψ+ψ(2S)→4μ, are studied. Backgrounds are estimated
             based on a hybrid approach involving Monte Carlo
             simulations and data-driven methods. Statistically
             significant excesses with respect to backgrounds dominated
             by the single parton scattering are seen in the di-J/ψ
             channel consistent with a narrow resonance at 6.9 GeV and a
             broader structure at lower mass. A statistically significant
             excess is also seen in the J/ψ+ψ(2S) channel. The fitted
             masses and decay widths of the structures are
             reported.},
   Doi = {10.1103/physrevlett.131.151902},
   Key = {fds373609}
}

@article{fds310342,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, M and Battistin,
             M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
             CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea,
             V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov,
             A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
             JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
             S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG},
   Title = {Observation of an excited Bc(±) meson state with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {113},
   Number = {21},
   Pages = {212004},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.113.212004},
   Abstract = {A search for excited states of the Bc(±) meson is performed
             using 4.9  fb(-1) of 7 TeV and 19.2  fb(-1) of 8 TeV
             pp collision data collected by the ATLAS experiment at the
             LHC. A new state is observed through its hadronic transition
             to the ground state, with the latter detected in the decay
             Bc(±)→J/ψπ(±). The state appears in the
             m(Bc(±)π(+)π(-))-m(Bc(±))-2m(π(±)) mass difference
             distribution with a significance of 5.2 standard deviations.
             The mass of the observed state is 6842±4±5  MeV, where
             the first error is statistical and the second is systematic.
             The mass and decay of this state are consistent with
             expectations for the second S-wave state of the Bc(±)
             meson, Bc(±)(2S).},
   Doi = {10.1103/physrevlett.113.212004},
   Key = {fds310342}
}

@article{fds307602,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu,
             E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee,
             P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behar Harpaz and S and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda,
             V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou,
             Y},
   Title = {Observation of associated near-side and away-side long-range
             correlations in sqrt[s(NN)]=5.02 TeV proton-lead collisions
             with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {18},
   Pages = {182302},
   Year = {2013},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.110.182302},
   Abstract = {Two-particle correlations in relative azimuthal angle (Δø)
             and pseudorapidity (Δη) are measured in sqrt[s(NN)] = 5.02
             TeV p+Pb collisions using the ATLAS detector at the LHC. The
             measurements are performed using approximately 1 μb(-1) of
             data as a function of transverse momentum (p(T)) and the
             transverse energy (ΣE(T)(Pb)) summed over 3.1 < η < 4.9 in
             the direction of the Pb beam. The correlation function,
             constructed from charged particles, exhibits a long-range (2
             < |Δ η | < 5) "near-side" (Δø ~ 0) correlation that
             grows rapidly with increasing ΣE(T)(Pb). A long-range
             "away-side" (Δø ~ π) correlation, obtained by subtracting
             the expected contributions from recoiling dijets and other
             sources estimated using events with small ΣE(T)(Pb), is
             found to match the near-side correlation in magnitude, shape
             (in Δη and Δø) and ΣE(T)(Pb) dependence. The resultant
             Δø correlation is approximately symmetric about π/2, and
             is consistent with a dominant cos2Δø modulation for all
             ΣE(T)(Pb) ranges and particle p(T).},
   Doi = {10.1103/physrevlett.110.182302},
   Key = {fds307602}
}

@article{fds348711,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carrillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copie, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas,
             J and Culbertson, R and Cully, JC and Cyr, D and DaRonco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and Barbaro, PD and Ceceo,
             SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and DiTuro,
             P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin,
             M and Freeman, JC and Frisch, HJ and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay,
             C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson,
             A and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths,
             M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hare, K and Hare, M and Harper, S and Harr, RF and Harris,
             RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
             A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
             S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee,
             SW and Lefevre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister,
             A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
             M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean,
             R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martinez, M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez,
             PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nagano, A and Naganoma, J and Nahn, S and Nakano, and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse,
             E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Porteil, X and Poukhov, O and Pounder, N and Prokoshin, F and Pronko, A and Proudfoot, J and Ptochos,
             F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ranjan,
             N and Rappoccio, S and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
             R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber,
             I},
   Title = {Observation of B s0 - B̄
             s0 oscillations},
   Journal = {Physical Review Letters},
   Volume = {97},
   Number = {24},
   Pages = {242003},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevLett.97.242003},
   Abstract = {We report the observation of B s0- B̄ s0 oscillations from
             a time-dependent measurement of the B s0-B̄ s0 oscillation
             frequency Δm s. Using a data sample of 1 fb -1 of pp
             collisions at √ = 1.96 TeV collected with the CDF II
             detector at the Fermilab Tevatron, we find signals of 5600
             fully reconstructed hadronic B s decays, 3100 partially
             reconstructed hadronic B s decays, and 61500 partially
             reconstructed semileptonic B s decays. We measure the
             probability as a function of proper decay time that the B s
             decays with the same, or opposite, flavor as the flavor at
             production, and we find a signal for B s0-B̄ s0
             oscillations. The probability that random fluctuations could
             produce a comparable signal is 8 × 10 -8, which exceeds 5σ
             significance. We measure Δm s = 17.77 ± 0.10(stat) ±
             0.07(syst) ps -1 and extract |V td/V ts| = 0.2060 ±
             0.0007(Δm s) -0.0060+0.0081 (Δm d + theor). © 2006 The
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.97.242003},
   Key = {fds348711}
}

@article{fds344671,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro,
             A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cresciolo, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
             PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and DiTuro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo,
             T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
             JP and Field, R and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
             I and Gallinaro, M and Galyardt, J and Garcia, JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris,
             N and Giolo, K and Giordani, M and Giromini, P and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and Gonzalez, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
             C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper,
             S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Heijboer, A and Heinemann, B and Heinrich, J and Herndon, M and Hidas,
             D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun,
             SY and Junk, TR and Kamon, T and Kang, J and Karchin, PE and Kato, Y and Kemp,
             Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim,
             YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee,
             YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister,
             A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
             M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
             H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto,
             A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse,
             E and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman, R and Orava,
             R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin,
             A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton, P and Rescigno, M and Richter, S and Rimondi,
             F and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers,
             E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz,
             A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman,
             D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti,
             A and Sinervo, P and Sisakyan, A and Sjolin, J},
   Title = {Observation of Bs0→ψ(2S) and measurement of the ratio of
             branching fractions B(Bs0→ψ(2S) /B(Bs0→J/ψ)},
   Journal = {Physical Review Letters},
   Volume = {96},
   Number = {23},
   Pages = {231801},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevLett.96.231801},
   Abstract = {We report the first observation of Bs0→ψ(2S) decay in
             pp̄ collisions at s= 1.96 TeV using 360 pb-1 of data
             collected by the CDF II detector at the Fermilab Tevatron.
             We observe 20.2±5.0 and 12.3±4.1 Bs0→ψ(2S) candidates,
             in ψ(2S)→μ+μ- and ψ(2S)→J/ψπ+π- decay modes,
             respectively. We present a measurement of the relative
             branching fraction B(Bs0→ψ(2S) /B(Bs0→J/ψ)=0.52±0.13(stat)±0.04(syst)±0.06(BR)
             using the ψ(2S)→μ+μ- decay mode. © 2006 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.96.231801},
   Key = {fds344671}
}

@article{fds347455,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
             M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
             E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
             M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
             KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
             U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
             D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
             BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
             S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V},
   Title = {Observation of Centrality-Dependent Acoplanarity for Muon
             Pairs Produced via Two-Photon Scattering in Pb+Pb Collisions
             at sqrt[s_{NN}]=5.02  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {121},
   Number = {21},
   Pages = {212301},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.121.212301},
   Abstract = {This Letter presents a measurement of γγ→μ^{+}μ^{-}
             production in Pb+Pb collisions recorded by the ATLAS
             detector at the Large Hadron Collider at
             sqrt[s_{NN}]=5.02  TeV with an integrated luminosity of
             0.49  nb^{-1}. The azimuthal angle and transverse
             momentum correlations between the muons are measured as a
             function of collision centrality. The muon pairs are
             produced from γγ through the interaction of the large
             electromagnetic fields of the nuclei. The contribution from
             background sources of muon pairs is removed using a template
             fit method. In peripheral collisions, the muons exhibit a
             strong back-to-back correlation consistent with previous
             measurements of muon pair production in ultraperipheral
             collisions. The angular correlations are observed to broaden
             significantly in central collisions. The modifications are
             qualitatively consistent with rescattering of the muons
             while passing through the hot matter produced in the
             collision.},
   Doi = {10.1103/physrevlett.121.212301},
   Key = {fds347455}
}

@article{fds307559,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kulkarni, N and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
             P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese,
             L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta,
             A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra,
             A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia,
             E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
             J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St
             Denis, R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
             P and Wallny, R and Wang, SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S},
   Title = {Observation of D⁰-D¯⁰ mixing using the CDF II
             detector.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {23},
   Pages = {231802},
   Year = {2013},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.111.231802},
   Abstract = {We measure the time dependence of the ratio of decay rates
             for D0→K(+)π(-) to the Cabibbo-favored decay
             D(0)→K(-)π(+). The charge conjugate decays are included.
             A signal of 3.3×10(4) D(*+)→π(+)D(0), D(0)→K(+)π(-)
             decays is obtained with D0 proper decay times between 0.75
             and 10 mean D0 lifetimes. The data were recorded with the
             CDF II detector at the Fermilab Tevatron and correspond to
             an integrated luminosity of 9.6  fb(-1) for pp¯
             collisions at √s=1.96  TeV. Assuming CP conservation,
             we search for D0-D¯0 mixing and measure the mixing
             parameters to be R(D)=(3.51±0.35)×10(-3),
             y'=(4.3±4.3)×10(-3), and x'2=(0.08±0.18)×10(-3). We
             report Bayesian probability intervals in the x'2-y' plane
             and find that the significance of excluding the no-mixing
             hypothesis is equivalent to 6.1 Gaussian standard
             deviations, providing the second observation of D0-D¯0
             mixing from a single experiment.},
   Doi = {10.1103/physrevlett.111.231802},
   Key = {fds307559}
}

@article{fds347181,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azoulay, AM and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines,
             JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi
             Gupta, D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee,
             S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
             G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous,
             S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall,
             A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund,
             O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock,
             I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni,
             A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer,
             F and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard,
             CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, V and Buschmann, E and Bussey,
             PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera
             Urbán, S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace,
             N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
             S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans,
             R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Carbone, RM and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney,
             RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio,
             A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ},
   Title = {Observation of Electroweak Production of a Same-Sign W Boson
             Pair in Association with Two Jets in pp Collisions at
             sqrt[s]=13  TeV with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {123},
   Number = {16},
   Pages = {161801},
   Year = {2019},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.123.161801},
   Abstract = {This Letter presents the observation and measurement of
             electroweak production of a same-sign W boson pair in
             association with two jets using 36.1  fb^{-1} of
             proton-proton collision data recorded at a center-of-mass
             energy of sqrt[s]=13  TeV by the ATLAS detector at the
             Large Hadron Collider. The analysis is performed in the
             detector fiducial phase-space region, defined by the
             presence of two same-sign leptons, electron or muon, and at
             least two jets with a large invariant mass and rapidity
             difference. A total of 122 candidate events are observed for
             a background expectation of 69±7 events, corresponding to
             an observed signal significance of 6.5 standard deviations.
             The measured fiducial signal cross section is
             σ^{fid}=2.89_{-0.48}^{+0.51}(stat)_{-0.28}^{+0.29}(syst)  fb.},
   Doi = {10.1103/physrevlett.123.161801},
   Key = {fds347181}
}

@article{fds374996,
   Author = {A.V. Kotwal and the ATLAS Collaboration},
   Title = {Observation of electroweak production of two jets and a
             Z-boson pair},
   Volume = {19},
   Pages = {237–253},
   Publisher = {Nature Physics},
   Year = {2023},
   Month = {February},
   ISSN = {Nature Physics},
   url = {http://dx.doi.org/https://doi.org/10.1038/s41567-022-01757-y},
   Doi = {https://doi.org/10.1038/s41567-022-01757-y},
   Key = {fds374996}
}

@article{fds362129,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
             SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury,
             KA and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
   Title = {Observation of electroweak production of two jets in
             association with an isolated photon and missing transverse
             momentum, and search for a Higgs boson decaying into
             invisible particles at 13 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {82},
   Number = {2},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2022},
   Month = {February},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09878-z},
   Abstract = {This paper presents a measurement of the electroweak
             production of two jets in association with a Zγ pair, with
             the Z boson decaying into two neutrinos. It also presents a
             search for invisible or partially invisible decays of a
             Higgs boson with a mass of 125 GeV produced through
             vector-boson fusion with a photon in the final state. These
             results use data from LHC proton–proton collisions at s =
             13 TeV collected with the ATLAS detector and corresponding
             to an integrated luminosity of 139 fb - 1. The event
             signature, shared by all benchmark processes considered for
             the measurements and searches, is characterized by a
             significant amount of unbalanced transverse momentum and a
             photon in the final state, in addition to a pair of forward
             jets. Electroweak Zγ production in association with two
             jets is observed in this final state with a significance of
             5.2 (5.1 expected) standard deviations. The measured
             fiducial cross-section for this process is 1.31 ± 0.29 fb.
             An observed (expected) upper limit of 0.37 (0.34-0.10+0.15)
             at 95% confidence level is set on the branching ratio of a
             125 GeV Higgs boson to invisible particles, assuming the
             Standard Model production cross-section. The signature is
             also interpreted in the context of decays of a Higgs boson
             into a photon and a dark photon. An observed (expected) 95%
             CL upper limit on the branching ratio for this decay is set
             at 0.018 (0.017-0.005+0.007), assuming the Standard Model
             production cross-section for a 125 GeV Higgs
             boson.},
   Doi = {10.1140/epjc/s10052-021-09878-z},
   Key = {fds362129}
}

@article{fds307945,
   Author = {Aaltonen, T and others},
   Title = {Observation of Electroweak Single Top-Quark
             Production},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {9},
   Pages = {092002},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.092002},
   Abstract = {We report the observation of single top-quark production
             using 3.2  fb-1 of pp̅ collision data with
             sqrt[s]=1.96  TeV collected by the Collider Detector at
             Fermilab. The significance of the observed data is 5.0
             standard deviations, and the expected sensitivity for
             standard model production and decay is in excess of 5.9
             standard deviations. Assuming mt=175  GeV/c2, we measure
             a cross section of 2.3-0.5+0.6(stat+syst)  pb, extract
             the CKM matrix-element value |Vtb|=0.91 &plusmn;
             0.11(stat+syst) &plusmn; 0.07(theory), and set the limit
             |Vtb|&gt;0.71 at the 95% C.L.},
   Doi = {10.1103/physrevlett.103.092002},
   Key = {fds307945}
}

@article{fds356590,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster,
             AJ},
   Title = {Observation of electroweak W±Z boson pair
             production in association with two jets in pp collisions at
             s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {793},
   Pages = {469-492},
   Year = {2019},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.05.012},
   Abstract = {An observation of electroweak W±Z production in association
             with two jets in proton–proton collisions is presented.
             The data collected by the ATLAS detector at the Large Hadron
             Collider in 2015 and 2016 at a centre-of-mass energy of s=13
             TeV are used, corresponding to an integrated luminosity of
             36.1fb−1. Events containing three identified leptons,
             either electrons or muons, and two jets are selected. The
             electroweak production of W±Z bosons in association with
             two jets is measured with an observed significance of 5.3
             standard deviations. A fiducial cross-section for
             electroweak production including interference effects and
             for a single leptonic decay mode is measured to be
             σWZjj−EW=0.57−0.13+0.14(stat.)−0.06+0.07(syst.)fb.
             Total and differential fiducial cross-sections of the sum of
             W±Zjj electroweak and strong productions for several
             kinematic observables are also measured.},
   Doi = {10.1016/j.physletb.2019.05.012},
   Key = {fds356590}
}

@article{fds307970,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
             A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
             A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey,
             P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni, GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes,
             D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani,
             M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
             S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Hamilton, A and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas,
             D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
             JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko,
             BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal,
             AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee, SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan,
             P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino,
             CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín,
             R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla
             Fernandez, P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Pagan Griso and S and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pinera, L and Pinfold, J and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
             J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla,
             A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer,
             B},
   Title = {Observation of exclusive charmonium production and
             gammagamma --> micro;{+}micro;{-} in pp[over] collisions at
             sqrt[s] = 1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {24},
   Pages = {242001},
   Year = {2009},
   Month = {June},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.102.242001},
   Abstract = {In CDF we have observed the reactions p + p[over] --> p + X
             + p[over], with X being a centrally produced J/psi, psi(2S),
             or chi_{c0}, and gammagamma-->micro;{+}micro;{-} in pp[over]
             collisions at sqrt[s] = 1.96 TeV. The event signature
             requires two oppositely charged central muons, and either no
             other particles or one additional photon detected. Exclusive
             vector meson production is as expected for elastic
             photoproduction, gamma + p --> J/psi(psi(2S)) + p, observed
             here for the first time in hadron-hadron collisions. We also
             observe exclusive chi_{c0} --> J/psi + gamma. The cross
             sections dsigma/dy|_{y = 0} for J/psi, psi(2S), and chi_{c0}
             are 3.92 +/- 0.25(stat) +/- 0.52(syst) nb, 0.53 +/-
             0.09(stat) +/- 0.10(syst) nb, and 76 +/- 10(stat) +/-
             10(syst) nb, respectively, and the continuum is consistent
             with QED. We put an upper limit on the cross section for
             Odderon exchange in exclusive J/psi production.},
   Doi = {10.1103/physrevlett.102.242001},
   Key = {fds307970}
}

@article{fds307713,
   Author = {Aaltonen, T and others},
   Title = {Observation of Exclusive Charmonium Production and
             γγ→μ+μ- in pp̅ Collisions at sqrt[s] =1.96
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {24},
   Pages = {242001},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.108.081801},
   Abstract = {In CDF we have observed the reactions p+p̅ →p+X+p̅ ,
             with X being a centrally produced J/ψ, ψ(2S), or χc0, and
             γγ→μ+μ- in pp̅ collisions at sqrt[s]=1.96  TeV.
             The event signature requires two oppositely charged central
             muons, and either no other particles or one additional
             photon detected. Exclusive vector meson production is as
             expected for elastic photoproduction, γ+p→J/ψ(ψ(2S))+p,
             observed here for the first time in hadron-hadron
             collisions. We also observe exclusive χc0→J/ψ+γ. The
             cross sections dσ / dy|y=0 for J/ψ, ψ(2S), and χc0 are
             3.92 &plusmn; 0.25(stat) &plusmn; 0.52(syst)  nb, 0.53
             &plusmn; 0.09(stat) &plusmn; 0.10(syst)  nb, and 76
             &plusmn; 10(stat) &plusmn; 10(syst)  nb, respectively,
             and the continuum is consistent with QED. We put an upper
             limit on the cross section for Odderon exchange in exclusive
             J/ψ production.},
   Doi = {10.1103/physrevlett.108.081801},
   Key = {fds307713}
}

@article{fds308061,
   Author = {Abulencia, and A, and others},
   Title = {Observation of exclusive electron positron production in
             hadron hadron collisions},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {11},
   Pages = {112001},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.112001},
   Abstract = {We present the first observation of exclusive e+e-
             production in hadron-hadron collisions, using p[overline p]
             collision data at sqrt(s)=1.96 TeV taken by the run II
             Collider Detector at Fermilab, and corresponding to an
             integrated luminosity of 532 pb-1. We require the absence of
             any particle signatures in the detector except for an
             electron and a positron candidate, each with transverse
             energy ET>5 GeV and pseudorapidity |eta|p+e+e-+[overline p]
             through two-photon exchange. The measured cross section is
             1.6-0.3+0.5(stat)$\pm$0.3(syst) pb. This agrees with the
             theoretical prediction of 1.71$\pm$0.01 pb.},
   Doi = {10.1103/physrevlett.98.112001},
   Key = {fds308061}
}

@article{fds372390,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel,
             A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed,
             WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh,
             B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
             AA and Cardoso, MA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler,
             A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA},
   Title = {Observation of four-top-quark production in the multilepton
             final state with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {6},
   Year = {2023},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11573-0},
   Abstract = {This paper presents the observation of four-top-quark (tt¯
             tt¯) production in proton-proton collisions at the LHC. The
             analysis is performed using an integrated luminosity of 140
             fb - 1 at a centre-of-mass energy of 13 TeV collected using
             the ATLAS detector. Events containing two leptons with the
             same electric charge or at least three leptons (electrons or
             muons) are selected. Event kinematics are used to separate
             signal from background through a multivariate discriminant,
             and dedicated control regions are used to constrain the
             dominant backgrounds. The observed (expected) significance
             of the measured tt¯ tt¯ signal with respect to the
             standard model (SM) background-only hypothesis is 6.1 (4.3)
             standard deviations. The tt¯ tt¯ production cross section
             is measured to be 22.5-5.5+6.6 fb, consistent with the SM
             prediction of 12.0 ± 2.4 fb within 1.8 standard deviations.
             Data are also used to set limits on the three-top-quark
             production cross section, being an irreducible background
             not measured previously, and to constrain the top-Higgs
             Yukawa coupling and effective field theory operator
             coefficients that affect tt¯ tt¯ production.},
   Doi = {10.1140/epjc/s10052-023-11573-0},
   Key = {fds372390}
}

@article{fds372120,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V},
   Title = {Observation of gauge boson joint-polarisation states in
             W±Z production from pp collisions at s=13 TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {843},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.137895},
   Abstract = {Measurements of joint-polarisation states of W and Z gauge
             bosons in W±Z production are presented. The data set used
             corresponds to an integrated luminosity of 139 fb−1 of
             proton–proton collisions at a centre-of-mass energy of 13
             TeV recorded by the ATLAS detector at the CERN Large Hadron
             Collider. The W±Z candidate events are reconstructed using
             leptonic decay modes of the gauge bosons into electrons and
             muons. The simultaneous pair-production of longitudinally
             polarised vector bosons is measured for the first time with
             a significance of 7.1 standard deviations. The measured
             joint helicity fractions integrated over the fiducial region
             are f00=0.067±0.010, f0T=0.110±0.029, fT0=0.179±0.023 and
             fTT=0.644±0.032, in agreement with the next-to-leading-order
             Standard Model predictions. Individual helicity fractions of
             the W and Z bosons are also measured and found to be
             consistent with joint helicity fractions within the expected
             amounts of correlation. Both the joint and individual
             helicity fractions are also measured separately in W+Z and
             W−Z events. Inclusive and differential cross sections for
             several kinematic observables sensitive to polarisation are
             presented.},
   Doi = {10.1016/j.physletb.2023.137895},
   Key = {fds372120}
}

@article{fds356661,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
   Title = {Observation of Higgs boson production in association with a
             top quark pair at the LHC with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {784},
   Pages = {173-191},
   Year = {2018},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.07.035},
   Abstract = {The observation of Higgs boson production in association
             with a top quark pair (tt¯H), based on the analysis of
             proton–proton collision data at a centre-of-mass energy of
             13 TeV recorded with the ATLAS detector at the Large Hadron
             Collider, is presented. Using data corresponding to
             integrated luminosities of up to 79.8 fb−1, and
             considering Higgs boson decays into bb¯, WW⁎, τ+τ−,
             γγ, and ZZ⁎, the observed significance is 5.8 standard
             deviations, compared to an expectation of 4.9 standard
             deviations. Combined with the tt¯H searches using a dataset
             corresponding to integrated luminosities of 4.5 fb−1 at 7
             TeV and 20.3 fb−1 at 8 TeV, the observed (expected)
             significance is 6.3 (5.1) standard deviations. Assuming
             Standard Model branching fractions, the total tt¯H
             production cross section at 13 TeV is measured to be 670 ±
             90 (stat.) −100+110 (syst.) fb, in agreement with the
             Standard Model prediction.},
   Doi = {10.1016/j.physletb.2018.07.035},
   Key = {fds356661}
}

@article{fds356638,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S},
   Title = {Observation of H→bb¯ decays and VH production with the
             ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {786},
   Pages = {59-86},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.09.013},
   Abstract = {A search for the decay of the Standard Model Higgs boson
             into a bb¯ pair when produced in association with a W or Z
             boson is performed with the ATLAS detector. The data,
             corresponding to an integrated luminosity of 79.8fb−1 were
             collected in proton–proton collisions during Run 2 of the
             Large Hadron Collider at a centre-of-mass energy of 13TeV.
             For a Higgs boson mass of 125GeV, an excess of events over
             the expected background from other Standard Model processes
             is found with an observed (expected) significance of 4.9
             (4.3) standard deviations. A combination with the results
             from other searches in Run 1 and in Run 2 for the Higgs
             boson in the bb¯ decay mode is performed, which yields an
             observed (expected) significance of 5.4 (5.5) standard
             deviations, thus providing direct observation of the Higgs
             boson decay into b-quarks. The ratio of the measured event
             yield for a Higgs boson decaying into bb¯ to the Standard
             Model expectation is 1.01±0.12(stat.)−0.15+0.16(syst.).
             Additionally, a combination of Run 2 results searching for
             the Higgs boson produced in association with a vector boson
             yields an observed (expected) significance of 5.3 (4.8)
             standard deviations.},
   Doi = {10.1016/j.physletb.2018.09.013},
   Key = {fds356638}
}

@article{fds347182,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
             Pereira, R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin,
             J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O and Arnold, H and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
             M and Atlay, NB and Atmani, H and Augsten, K and Avolio, G and Avramidou,
             R and Ayoub, MK and Azoulay, AM and Azuelos, G and Baca, MJ and Bachacou,
             H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bajic,
             M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura,
             AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barsov, S and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Berry, T and Berta, P and Bertella, C and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bitadze, A and Bittrich, C and Bjørke, K and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
             V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borecka-Bielska, HM and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
             WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock,
             I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burr, JTP and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, FC and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carter, JWS and Casado, MP and Casha, AF and Casper,
             DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro,
             NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, SK and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, B and Chen,
             C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Chu, MC and Chu, X and Chudoba, J},
   Title = {Observation of Light-by-Light Scattering in Ultraperipheral
             Pb+Pb Collisions with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {123},
   Number = {5},
   Pages = {052001},
   Year = {2019},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.123.052001},
   Abstract = {This Letter describes the observation of the light-by-light
             scattering process, γγ→γγ, in Pb+Pb collisions at
             sqrt[s_{NN}]=5.02  TeV. The analysis is conducted using
             a data sample corresponding to an integrated luminosity of
             1.73  nb^{-1}, collected in November 2018 by the ATLAS
             experiment at the LHC. Light-by-light scattering candidates
             are selected in events with two photons produced
             exclusively, each with transverse energy
             E_{T}^{γ}>3  GeV and pseudorapidity |η_{γ}|<2.4,
             diphoton invariant mass above 6 GeV, and small diphoton
             transverse momentum and acoplanarity. After applying all
             selection criteria, 59 candidate events are observed for a
             background expectation of 12±3 events. The observed excess
             of events over the expected background has a significance of
             8.2 standard deviations. The measured fiducial cross section
             is 78±13(stat)±7(syst)±3(lumi)  nb.},
   Doi = {10.1103/physrevlett.123.052001},
   Key = {fds347182}
}

@article{fds316844,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo,
             T},
   Title = {Observation of Long-Range Elliptic Azimuthal Anisotropies in
             sqrt[s]=13 and 2.76 TeV pp Collisions with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {116},
   Number = {17},
   Pages = {172301},
   Year = {2016},
   Month = {April},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.116.172301},
   Abstract = {ATLAS has measured two-particle correlations as a function
             of the relative azimuthal angle, Δϕ, and pseudorapidity,
             Δη, in sqrt[s]=13 and 2.76 TeV pp collisions at the LHC
             using charged particles measured in the pseudorapidity
             interval |η|<2.5. The correlation functions evaluated in
             different intervals of measured charged-particle
             multiplicity show a multiplicity-dependent enhancement at
             Δϕ∼0 that extends over a wide range of Δη, which has
             been referred to as the "ridge." Per-trigger-particle
             yields, Y(Δϕ), are measured over 2<|Δη|<5. For both
             collision energies, the Y(Δϕ) distribution in all
             multiplicity intervals is found to be consistent with a
             linear combination of the per-trigger-particle yields
             measured in collisions with less than 20 reconstructed
             tracks, and a constant combinatoric contribution modulated
             by cos(2Δϕ). The fitted Fourier coefficient, v_{2,2},
             exhibits factorization, suggesting that the ridge results
             from per-event cos(2ϕ) modulation of the single-particle
             distribution with Fourier coefficients v_{2}. The v_{2}
             values are presented as a function of multiplicity and
             transverse momentum. They are found to be approximately
             constant as a function of multiplicity and to have a p_{T}
             dependence similar to that measured in p+Pb and Pb+Pb
             collisions. The v_{2} values in the 13 and 2.76 TeV data
             are consistent within uncertainties. These results suggest
             that the ridge in pp collisions arises from the same or
             similar underlying physics as observed in p+Pb collisions,
             and that the dynamics responsible for the ridge has no
             strong sqrt[s] dependence.},
   Doi = {10.1103/physrevlett.116.172301},
   Key = {fds316844}
}

@article{fds307948,
   Author = {Aaltonen, T and others},
   Title = {Observation of New Charmless Decays of Bottom
             Hadrons},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {3},
   Pages = {031801},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.031801},
   Abstract = {We search for new charmless decays of neutral b hadrons to
             pairs of charged hadrons, using 1  fb-1 of data
             collected by the CDF II detector at the Fermilab Tevatron.
             We report the first observation of the Bs0→K-π+ decay and
             measure B(Bs0→K-π+)=(5.0 &plusmn; 0.7(stat) &plusmn;
             0.8(syst))×10-6. We also report the first observation of
             charmless b-baryon decays, and measure B(Λb0→pπ-)=(3.5
             &plusmn; 0.6(stat) &plusmn; 0.9(syst))×10-6 and
             B(Λb0→pK-)=(5.6 &plusmn; 0.8(stat) &plusmn;
             1.5(syst))×10-6. No evidence is found for other modes, and
             we set the limit B(Bs0→π+π-)&lt;1.2×10-6 at 90%
             C.L.},
   Doi = {10.1103/physrevlett.103.031801},
   Key = {fds307948}
}

@article{fds307532,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
             T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
             R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
             D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt,
             O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown,
             D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu, A and Calamba, A and Camacho-Pérez, E and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chakrabarti, S and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Cihangir, S and Claes, D and Clark, A and Clarke, C and Clutter, J and Convery, ME and Conway, J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and Cutts, D and Das, A and d'Ascenzo, N and Datta, M and Davies, G and de Barbaro, P and de Jong, SJ and De La
             Cruz-Burelo and E and Déliot, F and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov, SP and D'Errico, M and Desai, S and Deterre, C and DeVaughan, K and Devoto, F and Di Canto and A and Di Ruzza,
             B and Diehl, HT and Diesburg, M and Ding, PF and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, M and Driutti,
             A and Dubey, A and Dudko, LV and Duperrin, A and Dutt, S and Eads, M and Ebina, K and Edgar, R and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Erbacher, R and Errede, S and Esham, B and Evans, H and Evdokimov, VN and Farrington, S and Feng, L and Ferbel, T and Fernández Ramos and JP and Fiedler, F and Field, R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest, R and Fortner, M and Fox, H and Franklin, M and Freeman, JC and Frisch, H and Fuess, S and Funakoshi, Y and Galloni, C and Garbincius, PH and Garcia-Bellido, A and García-González, JA and Garfinkel, AF and Garosi, P and Gavrilov,
             V and Geng, W and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Golovanov, G and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grannis, PD and Greder, S and Greenlee, H and Grenier, G and Grinstein, S and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald, MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hahn, SR and Haley, J and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, M and Harel, A and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hauptman, JM and Hays, C and Hays, J and Head, T and Hebbeker, T and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De
             La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hildreth, MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen, B and Hogan, J and Hohlfeld, M and Holzbauer, JL and Hong, Z and Hopkins, W and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeon, EJ and Jeong, MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere,
             A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung,
             AW and Junk, TR and Juste, A and Kajfasz, E and Kambeitz, M and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kato, Y and Katsanos, I and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava, A and Kharzheev, YN and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim,
             YJ and Kim, YK and Kimura, N and Kirby, M and Kiselevich, I and Knoepfel,
             K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Kruse, M and Kuhr,
             T and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Laasanen, AT and Lammel, S and Lammers, S and Lancaster, M and Lannon,
             K and Latino, G and Lebrun, P and Lee, HS and Lee, JS and Lee, SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis, JD and Li, D and Li,
             H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Liu, H and Liu, Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lys, J and Lysak, R and Maciel, AKA and Madar, R and Madrak, R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G and Manousakis-Katsikakis, A and Mansour,
             J and Marchese, L and Margaroli, F and Marino, P and Martínez-Ortega,
             J and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McCarthy, R and McGivern, CL and McNulty, R and Mehta,
             A and Mehtala, P and Meijer, MM and Melnitchouk, A and Menezes, D and Mercadante, PG and Merkin, M and Mesropian, C and Meyer, A and Meyer, J and Miao, T and Miconi, F and Mietlicki, D and Mitra, A and Miyake, H and Moed,
             S and Moggi, N and Mondal, NK and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Mulhearn, M and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nagy, E and Nakano, I and Napier, A and Narain, M and Nayyar, R and Neal, HA and Negret, JP and Nett,
             J and Neu, C and Neustroev, P},
   Title = {Observation of s-channel production of single top quarks at
             the Tevatron.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {23},
   Pages = {231803},
   Year = {2014},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.112.231803},
   Abstract = {We report the first observation of single-top-quark
             production in the s channel through the combination of the
             CDF and D0 measurements of the cross section in
             proton-antiproton collisions at a center-of-mass energy of
             1.96 TeV. The data correspond to total integrated
             luminosities of up to 9.7 fb(-1) per experiment. The
             measured cross section is σ(s) = 1.29(-0.24)(+0.26) pb. The
             probability of observing a statistical fluctuation of the
             background to a cross section of the observed size or larger
             is 1.8 × 10(-10), corresponding to a significance of 6.3
             standard deviations for the presence of an s-channel
             contribution to the production of single-top
             quarks.},
   Doi = {10.1103/physrevlett.112.231803},
   Key = {fds307532}
}

@article{fds307921,
   Author = {Aaltonen, and T, and others},
   Title = {Observation of single top quark production and measurement
             of |$V_{tb}|$ with CDF},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {11},
   Pages = {112005},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.112005},
   Abstract = {We report the observation of electroweak single top quark
             production in 3.2fb⊃-1 of pp̄ collision data collected by
             the Collider Detector at Fermilab at √s=1.96TeV. Candidate
             events in the W+jets topology with a leptonically decaying W
             boson are classified as signal-like by four parallel
             analyses based on likelihood functions, matrix elements,
             neural networks, and boosted decision trees. These results
             are combined using a super discriminant analysis based on
             genetically evolved neural networks in order to improve the
             sensitivity. This combined result is further combined with
             that of a search for a single top quark signal in an
             orthogonal sample of events with missing transverse energy
             plus jets and no charged lepton. We observe a signal
             consistent with the standard model prediction but
             inconsistent with the background-only model by 5.0 standard
             deviations, with a median expected sensitivity in excess of
             5.9 standard deviations. We measure a production cross
             section of 2.3-0.5+0.6(stat+sys)pb, extract the value of the
             Cabibbo-Kobayashi-Maskawa matrix element |Vtb|=0.91-0.11+0.
             11(stat+sys)±0.07(theory), and set a lower limit |Vtb|>0.71
             at the 95%C.L., assuming mt=175GeV/c2.},
   Doi = {10.1103/PhysRevD.82.112005},
   Key = {fds307921}
}

@article{fds374211,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
             Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
             JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
             M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends,
             KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira,
             MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos,
             P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat,
             A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley,
             JR and Batool, B and Battaglia, M and Bauce, M and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
             P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov,
             VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
             M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer,
             JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi,
             G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya,
             DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel,
             O and Bielski, R and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov,
             VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden
             Madden, WD and Brendlinger, K and Brener, R and Brenner, L and Brenner,
             R and Bressler, S and Brickwedde, B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de
             Renstrom, PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov,
             O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
             EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
             AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
             Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo
             Garcia, L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi,
             E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen,
             SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov,
             MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
             BM and Clark, A and Clark, PJ and Clavijo Columbie and JM and Clawson,
             SE},
   Title = {Observation of Single-Top-Quark Production in Association
             with a Photon Using the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {131},
   Number = {18},
   Pages = {181901},
   Year = {2023},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.131.181901},
   Abstract = {This Letter reports the observation of single top quarks
             produced together with a photon, which directly probes the
             electroweak coupling of the top quark. The analysis uses
             139  fb^{-1} of 13 TeV proton-proton collision data
             collected with the ATLAS detector at the Large Hadron
             Collider. Requiring a photon with transverse momentum larger
             than 20 GeV and within the detector acceptance, the
             fiducial cross section is measured to be
             688±23(stat) _{-71}^{+75}(syst)  fb, to be compared
             with the standard model prediction of 515_{-42}^{+36}  fb
             at next-to-leading order in QCD.},
   Doi = {10.1103/physrevlett.131.181901},
   Key = {fds374211}
}

@article{fds307700,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni,
             G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
             Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland,
             W},
   Title = {Observation of spin correlation in tt¯ events from pp
             collisions at √s=7 TeV using the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {21},
   Pages = {212001},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.212001},
   Abstract = {A measurement of spin correlation in tt[over ¯] production
             is reported using data collected with the ATLAS detector at
             the LHC, corresponding to an integrated luminosity of 2.1
             fb(-1). Candidate events are selected in the dilepton
             topology with large missing transverse energy and at least
             two jets. The difference in azimuthal angle between the two
             charged leptons in the laboratory frame is used to extract
             the correlation between the top and antitop quark spins. In
             the helicity basis the measured degree of correlation
             corresponds to A(helicity)=0.40(-0.08)(+0.09), in agreement
             with the next-to-leading-order standard model prediction.
             The hypothesis of zero spin correlation is excluded at 5.1
             standard deviations.},
   Doi = {10.1103/physrevlett.108.212001},
   Key = {fds307700}
}

@article{fds307839,
   Author = {Aaltonen, and T, and al, E},
   Title = {Observation of the $\Xi_{b}^{0}$ Baryon},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {10},
   Pages = {102001},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.102001},
   Abstract = {The observation of the bottom, strange baryon Ξ(b)(0)
             through the decay chain Ξ(b)(0)→Ξ(c)(+)π-, where
             ΞΞ(c)(+)→Ξ- π+ π+, Ξ-→Λπ-, and Λ→pπ-, is
             reported by using data corresponding to an integrated
             luminosity of 4.2  fb(-1) from pp collisions at square
             root(s)=1.96  TeV recorded with the Collider Detector at
             Fermilab. A signal of 25.3(-5.4)(+5.6) candidates is
             observed whose probability of arising from a background
             fluctuation is 3.6×10(-12), corresponding to 6.8 gaussian
             standard deviations. The Ξ(b)(0) mass is measured to be
             5787.8±5.0(stat)±1.3(syst)  MeV/c2. In addition, the
             Ξ(b)- baryon is observed through the process
             Ξ(b)-→Ξ(c)(0)π-, where Ξ(c)(0)→Ξ- π+, Ξ-→Λπ-,
             and Λ→pπ-.},
   Doi = {10.1103/PhysRevLett.107.102001},
   Key = {fds307839}
}

@article{fds351556,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH},
   Title = {Observation of the associated production of a top quark and
             a Z boson in pp collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {7},
   Year = {2020},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2020)124},
   Abstract = {Single top-quark production in association with a Z boson,
             where the Z boson decays to a pair of charged leptons, is
             measured in the trilepton channel. The proton-proton
             collision data collected by the ATLAS experiment from 2015
             to 2018 at a centre-of-mass energy of 13 TeV are used,
             corresponding to an integrated luminosity of 139 fb−1.
             Events containing three isolated charged leptons (electrons
             or muons) and two or three jets, one of which is identified
             as containing a b-hadron, are selected. The main backgrounds
             are from tt¯ Z and diboson production. Neural networks are
             used to improve the background rejection and extract the
             signal. The measured cross-section for tℓ+ℓ−q
             production, including non-resonant dilepton pairs with
             mℓ+ℓ−> 30 GeV, is 97 ± 13 (stat.) ± 7 (syst.) fb,
             consistent with the Standard Model prediction. [Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP07(2020)124},
   Key = {fds351556}
}

@article{fds307833,
   Author = {Aaltonen, TEA},
   Title = {Observation of the Baryonic Flavor-Changing Neutral Current
             Decay $\Lambda_{b}^{0}\rightarrow\Lambda\mu^{+}\mu^{-}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {20},
   Pages = {201802},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.201802},
   Abstract = {We report the first observation of the baryonic
             flavor-changing neutral current decay Λ(b)(0)→Λμ(+)μ(-)
             with 24 signal events and a statistical significance of 5.8
             Gaussian standard deviations. This measurement uses a pp
             collisions data sample corresponding to 6.8 fb(-1) at √s =
             1.96 TeV collected by the CDF II detector at the Tevatron
             collider. The total and differential branching ratios for
             Λ(b)(0)→Λμ(+)μ(-) are measured. We find
             B(Λ(b)(0)→Λμ(+)μ(-))=[1.73 ± 0.42(stat) ± (syst)] ×
             10(-6). We also report the first measurement of the
             differential branching ratio of B(s)(0)→ϕμ(+)μ(-),
             using 49 signal events. In addition, we report branching
             ratios for B(+)→K(+)μ(+)μ(-), B(0)→K(0)μ(+)μ(-), and
             B→K(*)(892)μ(+)μ(-) decays.},
   Doi = {10.1103/PhysRevLett.107.201802},
   Key = {fds307833}
}

@article{fds361694,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov,
             A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Lorenzo,
             GD and Dell'Orso, M and Demortier, L and Deng, J and Deninno, M and Pedis,
             DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes,
             D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
             C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker,
             A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun,
             SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato,
             Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim,
             YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson,
             B and Ko, BR and Koay, SA and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus, J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone,
             S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, RS and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
             D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
             P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli,
             F and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Griso,
             SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic,
             V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
             L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó,
             O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro,
             A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
             AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima,
             M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ},
   Title = {Observation of the decay Bc±→J/ψπ± and measurement of
             the Bc± mass},
   Journal = {Physical Review Letters},
   Volume = {100},
   Number = {18},
   Pages = {182002},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevLett.100.182002},
   Abstract = {The Bc± meson is observed through the decay Bc±→J/
             ψπ±, in data corresponding to an integrated luminosity of
             2.4fb-1 recorded by the Collider Detector at Fermilab II
             detector at the Fermilab Tevatron. A signal of 108±15
             candidates is observed, with a significance that exceeds
             8σ. The mass of the Bc± meson is measured to be
             6275.6±2.9(stat)±2.5(syst)MeV/c2. © 2008 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.100.182002},
   Key = {fds361694}
}

@article{fds308066,
   Author = {Aaltonen, T and Abulencia, A and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev,
             K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Behari,
             S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and DaRonco, S and Datta, M and D'Auria, S and Davies, T and Dagenhart, D and de Barbaro, P and De
             Cecco, S and Deisher, A and De Lentdecker and G and De Lorenzo and G and Dell'Orso, M and Delli Paoli and F and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Dörr,
             C and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron,
             J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
             M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro,
             M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani,
             M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
             da Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
             RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson,
             C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl,
             D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel,
             U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraan, AC and Kraus,
             J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
             C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
             J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli, F and Marginean,
             R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty,
             R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel,
             P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles,
             J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher,
             G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moon, CS and Moore,
             R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou,
             A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
             R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov,
             A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar,
             S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
             AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima,
             M and Shochet, M and Shon, Y},
   Title = {Observation of the Heavy Baryons Sigma b and Sigma
             b*.},
   Journal = {Physical review letters},
   Volume = {99},
   Number = {20},
   Pages = {202001},
   Year = {2007},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.99.202001},
   Abstract = {We report an observation of new bottom baryons produced in
             pp collisions at the Tevatron. Using 1.1 fb(-1) of data
             collected by the CDF II detector, we observe four Lambda b 0
             pi+/- resonances in the fully reconstructed decay mode
             Lambda b 0-->Lambda c + pi-, where Lambda c+-->pK* pi+. We
             interpret these states as the Sigma b(*)+/- baryons and
             measure the following masses: m Sigma b+=5807.8 -2.2
             +2.0(stat.)+/-1.7(syst.) MeV/c2, m Sigma b-
             =5815.2+/-1.0(stat.)+/-1.7(syst.) MeV/c2, and m(Sigma
             b*)-m(Sigma b)=21.2-1.9 +2.0(stat.)-0.3+0.4(syst.)
             MeV/c2.},
   Doi = {10.1103/physrevlett.99.202001},
   Key = {fds308066}
}

@article{fds308164,
   Author = {Acosta, D and Affolder, T and Ahn, MH and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and Barbaro-Galtieri, A and Barker, G and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini,
             G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov,
             S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett,
             K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura,
             P and Campanelli, M and Campbell, M and Canepa, A and Carlsmith, D and Carron, S and Carosi, R and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen,
             C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chu, ML and Chung, JY and Chung,
             WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, MN and Connolly, A and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cranshaw, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and DaRonco, S and D'Auria, S and Barbaro, PD and Cecco,
             SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers,
             S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and Doksus, P and Dominguez, A and Donati,
             S and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
             N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Frisch, H and Fujii, Y and Furic, I and Gaijar, A and Gallas, A and Gallinaro, M and Galyardt, J and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerchtein, E and Gerdes, DW and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hall, C and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke,
             M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman,
             KD and Holloway, A and Hou, S and Houlden, MA and Huang, Y and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
             H and Jones, M and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim,
             TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov,
             K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer,
             A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis,
             JD and Li, K and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loken, J and Loreti,
             M and Loverre, P and Lucchesi, D and Lukens, P and Lyons, L and Lys, J and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, A and Martin, M and Martin, V and Martinez, M and Maruyama, T and Matsunaga, H and Mattson,
             M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, R and Menzemer, S and Menzione, A and Merkel,
             P and Mesropian, C and Messina, A and Meyer, A and Miao, T and Miladinovic,
             N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mishina, M and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Moore, R and Morello, M and Moulik, T and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, AS and Nigmanov, T and Nodulman, L and Oesterberg, K and Ogawa, T and Oh, S and Oh, YD and Ohsugi, T and Oishi, R and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari,
             F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray,
             H and Reichold, A and Rekovic, V and Renton, P and Rescigno, M and Rimondi,
             F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni,
             A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro,
             A and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shon, Y and Sidoti, A and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba, A and Slaughter, AJ and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Somalwar, SV and Spalding, J and Spezziga, M and Spiegel, L and Spinella, F and Spiropulu, M and Squillacioti, P and Stadie, H and Stelzer, B and Stelzer-Chilton, O and Strologas, J and Stuart, D and Sukhanov, A and Sumorok,
             K},
   Title = {Observation of the narrow state X(3872) →
             J/ψπ+π- in p̄p collisions at √s
             = 1.96 TeV},
   Journal = {Physical Review Letters},
   Volume = {93},
   Number = {7},
   Pages = {072001-1-072001-6},
   Year = {2004},
   url = {http://dx.doi.org/10.1103/PhysRevLett.93.072001},
   Abstract = {The observation of a state consistent with X(3872) decaying
             into J/ψπ+π- was reported. The X(3872) mass was measured
             to be 3871.3±0.7(stat)±0.4(syst)MeV/c2 from a sample of
             730±90 candidates. The observed width was consistent with
             the detector resolution. The results were found to be
             converging well with the measurements by the Belle
             Collaboration using b± decays.},
   Doi = {10.1103/PhysRevLett.93.072001},
   Key = {fds308164}
}

@article{fds307628,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chou, JP and Chokheli,
             D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza,
             B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Funakoshi, Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hopkins, W and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leone, S and Lewis, JD and Limosani, A and Lipeles,
             E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys,
             J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty,
             R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki,
             D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore,
             R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia,
             E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro,
             A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi,
             G and Wagner, P and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams,
             HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers,
             S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato,
             D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Observation of the production of a W boson in association
             with a single charm quark.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {7},
   Pages = {071801},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.110.071801},
   Abstract = {The first observation of the production of a W boson with a
             single charm quark (c) jet in pp[over ¯] collisions at
             √s=1.96  TeV is reported. The analysis uses data
             corresponding to 4.3  fb(-1), recorded with the CDF II
             detector at the Fermilab Tevatron. Charm quark candidates
             are selected through the identification of an electron or
             muon from charm-hadron semileptonic decay within a hadronic
             jet, and a Wc signal is observed with a significance of 5.7
             standard deviations. The production cross section
             σ(Wc)(p(Tc)>20  GeV/c,|η(c)|<1.5)×B(W→ℓν) is
             measured to be 13.6(-3.1)(+3.4)  pb and is in agreement
             with theoretical expectations. From this result the
             magnitude of the quark-mixing matrix element V(cs) is
             derived, |V(cs)|=1.08±0.16 along with a lower limit of
             |V(cs)|>0.71 at the 95% confidence level, assuming that the
             Wc production through c to s quark coupling is
             dominant.},
   Doi = {10.1103/physrevlett.110.071801},
   Key = {fds307628}
}

@article{fds356741,
   Author = {Aaltonen, T and Alvarez Gonzálezv and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Braua, B and Brigliadori, L and Brisuda,
             A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell,
             M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, CY and Chertok, M and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway,
             J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and Ascenzo, N},
   Title = {Observation of the y (4 1 4 0) structure in the J/mass
             spectrum in B ±±→K ± decays},
   Journal = {Modern Physics Letters A},
   Volume = {32},
   Number = {26},
   Year = {2017},
   Month = {August},
   url = {http://dx.doi.org/10.1142/S0217732317501395},
   Abstract = {The observation of the Y (4140) structure in B± →
             J/ΨφK± decays produced in pp collisions at √ s = 1.96
             TeV is reported with a statistical significance greater than
             5 standard deviations. A fit to the J/Ψφ mass spectrum is
             performed assuming the presence of a Breit-Wigner resonance.
             The fit yields a signal of 19 ± 6 (stat) ± 3 (syst)
             resonance events, and resonance mass and width of 4143.4+2.9
             -3.0 (stat)±0.6 (syst) MeV/c2 and 15.3+10.4 -6.1
             (stat)±2.5 (syst) MeV/c2, respectively. The parameters of
             this resonancelike structure are consistent with values
             reported from an earlier CDF analysis.},
   Doi = {10.1142/S0217732317501395},
   Key = {fds356741}
}

@article{fds373610,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
             Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
             PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baron
             Moreno, DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco
             Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
             M and Bauce, M and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
             K and Becot, C and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos,
             P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun,
             D and Bendebba, F and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram,
             IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biglietti, M and Billoud,
             TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Bisceglie,
             E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden
             Madden, WD and Brendlinger, K and Brener, R and Brenner, L and Brenner,
             R and Bressler, S and Brickwedde, B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de
             Renstrom, PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov,
             O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
             EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
             AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
             Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo
             Garcia, L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi,
             E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen,
             SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
             YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro,
             V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark, A and Clark, PJ and Clavijo
             Columbie, JM},
   Title = {Observation of the γγ→ττ Process in Pb+Pb Collisions
             and Constraints on the τ-Lepton Anomalous Magnetic Moment
             with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {131},
   Number = {15},
   Pages = {151802},
   Year = {2023},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.131.151802},
   Abstract = {This Letter reports the observation of τ-lepton-pair
             production in ultraperipheral lead-lead collisions
             Pb+Pb→Pb(γγ→ττ)Pb and constraints on the τ-lepton
             anomalous magnetic moment a_{τ}. The dataset corresponds to
             an integrated luminosity of 1.44  nb^{-1} of LHC Pb+Pb
             collisions at sqrt[s_{NN}]=5.02  TeV recorded by the
             ATLAS experiment in 2018. Selected events contain one muon
             from a τ-lepton decay, an electron or charged-particle
             track(s) from the other τ-lepton decay, little additional
             central-detector activity, and no forward neutrons. The
             γγ→ττ process is observed in Pb+Pb collisions with a
             significance exceeding 5 standard deviations and a signal
             strength of μ_{ττ}=1.03_{-0.05}^{+0.06} assuming the
             standard model value for a_{τ}. To measure a_{τ}, a
             template fit to the muon transverse-momentum distribution
             from τ-lepton candidates is performed, using a dimuon
             (γγ→μμ) control sample to constrain systematic
             uncertainties. The observed 95% confidence-level interval
             for a_{τ} is -0.057<a_{τ}<0.024.},
   Doi = {10.1103/physrevlett.131.151802},
   Key = {fds373610}
}

@article{fds307989,
   Author = {Aaltonen, T and others},
   Title = {Observation of the Ωb- baryon and measurement of the
             properties of the Ξb- and Ωb- baryons},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {7},
   Pages = {072003},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.072003},
   Abstract = {We report the observation of the bottom, doubly-strange
             baryon Ωb- through the decay chain Ωb-→J/ψΩ-, where
             J/ψ→μ+μ-, Ω-→ΛK-, and Λ→pπ-, using
             4.2  fb-1 of data from pp̅ collisions at
             sqrt[s]=1.96  TeV, and recorded with the Collider
             Detector at Fermilab. A signal is observed whose probability
             of arising from a background fluctuation is 4.0×10-8, or
             5.5 Gaussian standard deviations. The Ωb- mass is measured
             to be 6054.4 &plusmn; 6.8(stat) &plusmn;
             0.9(syst)  MeV/c2. The lifetime of the Ωb- baryon is
             measured to be 1.13-0.40+0.53(stat) &plusmn;
             0.02(syst)  ps. In addition, for the Ξb- baryon we
             measure a mass of 5790.9 &plusmn; 2.6(stat) &plusmn;
             0.8(syst)  MeV/c2 and a lifetime of 1.56-0.25+0.27(stat)
             &plusmn; 0.02(syst)  ps. Under the assumption that the
             Ξb- and Ωb- are produced with similar kinematic
             distributions to the Λb0 baryon, we find
             σ(Ξb-)B(Ξb-→J/ψΞ-) / σ(Λb0)B(Λb0→J/ψΛ)=0.167-0.025+0.037(stat)
             &plusmn; 0.012(syst) and σ(Ωb-)B(Ωb-→J/ψΩ-) /
             σ(Λb0)B(Λb0→J/ψΛ)=0.045-0.012+0.017(stat) &plusmn;
             0.004(syst) for baryons produced with transverse momentum in
             the range of 6--20  GeV/c.},
   Doi = {10.1103/PhysRevD.80.072003},
   Key = {fds307989}
}

@article{fds310294,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Observation of top-quark pair production in association with
             a photon and measurement of the t t ¯ γ production cross
             section in pp collisions at √s =7 TeV using the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.072007},
   Abstract = {A search is performed for top-quark pairs (tt¯) produced
             together with a photon (γ) with transverse energy greater
             than 20 GeV using a sample of tt¯ candidate events in final
             states with jets, missing transverse momentum, and one
             isolated electron or muon. The data set used corresponds to
             an integrated luminosity of 4.59 fb-1 of proton-proton
             collisions at a center-of-mass energy of 7 TeV recorded by
             the ATLAS detector at the CERN Large Hadron Collider. In
             total, 140 and 222 tt¯γ candidate events are observed in
             the electron and muon channels, to be compared to the
             expectation of 79±26 and 120±39 non-tt¯γ background
             events, respectively. The production of tt¯γ events is
             observed with a significance of 5.3 standard deviations away
             from the null hypothesis. The tt¯γ production cross
             section times the branching ratio (BR) of the single-lepton
             decay channel is measured in a fiducial kinematic region
             within the ATLAS acceptance. The measured value is
             σtt¯γfid×BR=63±8(stat)-13+17(syst)±1(lumi) fb per
             lepton flavor, in good agreement with the leading-order
             theoretical calculation normalized to the
             next-to-leading-order theoretical prediction of 48±10
             fb.},
   Doi = {10.1103/PhysRevD.91.072007},
   Key = {fds310294}
}

@article{fds366921,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler,
             A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai,
             K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Austrup, VA and Avner, G and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baroncelli,
             A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos,
             P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat,
             A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley,
             JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
             F and Bechtle, P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli,
             M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
             L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertram, IA and Bessidskaia Bylund and O and Bethke, S and Betti, A and Bevan, AJ and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler, S and Brickwedde,
             B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks,
             WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko,
             D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard,
             CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler,
             JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez,
             CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
             JCJ and Cardillo, F and Carducci, G and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron,
             S and Carquin, E and Carrá, S and Carratta, G and Carter, JWS and Carter,
             TM and Casadei, D and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen,
             H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark, A and Clark, PJ and Clavijo
             Columbie, JM and Clawson, SE and Clement, C and Clissa, L and Coadou,
             Y},
   Title = {Observation of WWW Production in pp Collisions at
             sqrt[s]=13  TeV with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {129},
   Number = {6},
   Pages = {061803},
   Year = {2022},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.129.061803},
   Abstract = {This Letter reports the observation of WWW production and a
             measurement of its cross section using 139  fb^{-1} of
             proton-proton collision data recorded at a center-of-mass
             energy of 13 TeV by the ATLAS detector at the Large Hadron
             Collider. Events with two same-sign leptons (electrons or
             muons) and at least two jets, as well as events with three
             charged leptons, are selected. A multivariate technique is
             then used to discriminate between signal and background
             events. Events from WWW production are observed with a
             significance of 8.0 standard deviations, where the
             expectation is 5.4 standard deviations. The inclusive WWW
             production cross section is measured to be
             820±100 (stat)±80 (syst)  fb, approximately 2.6
             standard deviations from the predicted cross section of
             511±18  fb calculated at next-to-leading-order QCD and
             leading-order electroweak accuracy.},
   Doi = {10.1103/physrevlett.129.061803},
   Key = {fds366921}
}

@article{fds375334,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
             J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
             Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
             GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
             M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
             JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
             Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
             PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour,
             G and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr,
             AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
             M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano
             Hurrell, LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
             F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov,
             VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
             M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir,
             M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal,
             J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
             R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
             PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
             CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo
             Vazquez, CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir,
             O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
             Bret, M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone,
             A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin,
             E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo,
             FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
             J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
             A},
   Title = {Observation of WZγ Production in pp Collisions at
             sqrt[s]=13  TeV with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {132},
   Number = {2},
   Pages = {021802},
   Year = {2024},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.132.021802},
   Abstract = {This Letter reports the observation of WZγ production and a
             measurement of its cross section using 140.1±1.2  fb^{-1}
             of proton-proton collision data recorded at a center-of-mass
             energy of 13 TeV by the ATLAS detector at the Large Hadron
             Collider. The WZγ production cross section, with both the W
             and Z bosons decaying leptonically, pp→WZγ→ℓ^{'}^{±}νℓ^{+}ℓ^{-}γ
             (ℓ^{(^{'})}=e, μ), is measured in a fiducial phase-space
             region defined such that the leptons and the photon have
             high transverse momentum and the photon is isolated. The
             cross section is found to be 2.01±0.30(stat)±0.16(syst)  fb.
             The corresponding standard model predicted cross section
             calculated at next-to-leading order in perturbative quantum
             chromodynamics and at leading order in the electroweak
             coupling constant is 1.50±0.06  fb. The observed
             significance of the WZγ signal is 6.3σ, compared with an
             expected significance of 5.0σ.},
   Doi = {10.1103/physrevlett.132.021802},
   Key = {fds375334}
}

@article{fds375987,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
             J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
             Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
             GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
             M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
             JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
             C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
             KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
   Title = {Observation of Wγγ triboson production in proton-proton
             collisions at s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {848},
   Year = {2024},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.138400},
   Abstract = {This letter reports the observation of W(ℓν)γγ
             production in proton-proton collisions. This measurement
             uses the full Run 2 sample of events recorded at a
             center-of-mass energy of s=13 TeV by the ATLAS detector at
             the LHC, corresponding to an integrated luminosity of 140
             fb−1. Events with a leptonically-decaying W boson and at
             least two photons are considered. The background-only
             hypothesis is rejected with an observed and expected
             significance of 5.6 standard deviations. The inclusive
             fiducial production cross section of W(eν)γγ and
             W(μν)γγ events is measured to be σfid=13.8±1.1(stat)+2.1−2.0(syst)±0.1(lumi)
             fb, in agreement with the Standard Model
             prediction.},
   Doi = {10.1016/j.physletb.2023.138400},
   Key = {fds375987}
}

@article{fds346193,
   Author = {Sangwan, BR and Kotwal, A and Verma, AK},
   Title = {Occupational Exposure to Blood and Body Fluids amongst
             Health Care Workers in a Teaching Hospital of the Armed
             Forces.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {67},
   Number = {1},
   Pages = {21-24},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1016/s0377-1237(11)80006-7},
   Abstract = {<h4>Background</h4>Health care workers (HCWs) are at risk of
             infection with blood-borne viruses in the course of their
             work. Over 90% of these infections are occurring in
             low-income countries and most are preventable. However, the
             situation in the Armed Forces hospitals has always been
             thought to be much better than the public health facilities
             in India. The focus of the study was on assessing the
             exposure frequency amongst HCWs in a teaching hospital in
             the Armed Forces.<h4>Methods</h4>A cross-sectional survey
             amongst HCWs involved in collecting blood samples and
             administering injections in all wards of the hospital was
             conducted. Selection of study participants was by simple
             random sampling. A pre-tested questionnaire was administered
             by unlinked, anonymous method.<h4>Result</h4>Total sample
             studied was 70. The proportion of HCWs experiencing exposure
             to blood body fluid splash (BBF) and needlestick injury
             (NSI) during last one week was 47.1 % and 31.43 %,
             respectively. The incidence density of BBF exposure was
             537.14 per 100 person years and that of NSI episodes was
             228.57 per 100 person years. The reasons for not using
             personal protective equipment (PPE) ranged from busy
             schedule (37.14%), non use of PPE by co-workers (67.14%),
             emergencies (91.43%) risk that patients may get offended by
             PPE use by HCWs (27.14%) to discomfort while using PPE
             (24.29%). All components of PPE were available as per only
             34.29 percent.<h4>Conclusion</h4>The high level of
             occupational exposure to blood and body fluids and
             consequent risk of infection amongst a group of HCWs in the
             Armed Forces highlights the urgent need for interventions to
             enhance the occupational safety of workers.},
   Doi = {10.1016/s0377-1237(11)80006-7},
   Key = {fds346193}
}

@article{fds316846,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O},
   Title = {Operation and performance of the ATLAS semiconductor
             tracker},
   Journal = {Journal of Instrumentation},
   Volume = {9},
   Number = {8},
   Pages = {P08009-P08009},
   Publisher = {IOP Publishing},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1748-0221/9/08/P08009},
   Abstract = {The semiconductor tracker is a silicon microstrip detector
             forming part of the inner tracking system of the ATLAS
             experiment at the LHC. The operation and performance of the
             semiconductor tracker during the first years of LHC running
             are described. More than 99% of the detector modules were
             operational during this period, with an average intrinsic
             hit efficiency of (99.74±0.04)%. The evolution of the noise
             occupancy is discussed, and measurements of the Lorentz
             angle, d-ray production and energy loss presented. The
             alignment of the detector is found to be stable at the
             few-micron level over long periods of time. Radiation damage
             measurements, which include the evolution of detector
             leakage currents, are found to be consistent with
             predictions and are used in the verification of radiation
             background simulations.},
   Doi = {10.1088/1748-0221/9/08/P08009},
   Key = {fds316846}
}

@article{fds362042,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
             SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Verzini,
             MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso,
             S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C},
   Title = {Operation and performance of the ATLAS semiconductor tracker
             in LHC Run 2},
   Journal = {Journal of Instrumentation},
   Volume = {17},
   Number = {1},
   Year = {2022},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1748-0221/17/01/P01013},
   Abstract = {The semiconductor tracker (SCT) is one of the tracking
             systems for charged particles in the ATLAS detector. It
             consists of 4088 silicon strip sensor modules. During Run 2
             (2015-2018) the Large Hadron Collider delivered an
             integrated luminosity of 156 fb−1 to the ATLAS experiment
             at a centre-of-mass proton-proton collision energy of 13
             TeV. The instantaneous luminosity and pile-up conditions
             were far in excess of those assumed in the original design
             of the SCT detector. Due to improvements to the data
             acquisition system, the SCT operated stably throughout Run
             2. It was available for 99.9% of the integrated luminosity
             and achieved a data-quality efficiency of 99.85%. Detailed
             studies have been made of the leakage current in SCT modules
             and the evolution of the full depletion voltage, which are
             used to study the impact of radiation damage to the
             modules.},
   Doi = {10.1088/1748-0221/17/01/P01013},
   Key = {fds362042}
}

@article{fds347483,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Pereira, RA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey,
             AJ and Baines, JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Gupta, DB and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura,
             AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
             G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous,
             S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot,
             C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
             M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Brown, H and Bruckman de
             Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler,
             JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
             S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Argos, FC and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
             R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
             YS},
   Title = {Operation and performance of the ATLAS Tile Calorimeter in
             Run 1.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {12},
   Pages = {987},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-6374-z},
   Abstract = {The Tile Calorimeter is the hadron calorimeter covering the
             central region of the ATLAS experiment at the Large Hadron
             Collider. Approximately 10,000 photomultipliers collect
             light from scintillating tiles acting as the active material
             sandwiched between slabs of steel absorber. This paper gives
             an overview of the calorimeter's performance during the
             years 2008-2012 using cosmic-ray muon events and
             proton-proton collision data at centre-of-mass energies of 7
             and 8 TeV with a total integrated luminosity of nearly
             30 fb - 1 . The signal reconstruction methods, calibration
             systems as well as the detector operation status are
             presented. The energy and time calibration methods performed
             excellently, resulting in good stability of the calorimeter
             response under varying conditions during the LHC Run 1.
             Finally, the Tile Calorimeter response to isolated muons and
             hadrons as well as to jets from proton-proton collisions is
             presented. The results demonstrate excellent performance in
             accord with specifications mentioned in the Technical Design
             Report.},
   Doi = {10.1140/epjc/s10052-018-6374-z},
   Key = {fds347483}
}

@article{fds356048,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
   Title = {Optimisation of large-radius jet reconstruction for the
             ATLAS detector in 13 TeV proton–proton
             collisions},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {4},
   Year = {2021},
   Month = {April},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09054-3},
   Abstract = {Jet substructure has provided new opportunities for searches
             and measurements at the LHC, and has seen continuous
             development since the optimization of the large-radius jet
             definition used by ATLAS was performed during Run 1. A range
             of new inputs to jet reconstruction, pile-up mitigation
             techniques and jet grooming algorithms motivate an
             optimisation of large-radius jet reconstruction for ATLAS.
             In this paper, this optimisation procedure is presented, and
             the performance of a wide range of large-radius jet
             definitions is compared. The relative performance of these
             jet definitions is assessed using metrics such as their
             pileup stability, ability to identify hadronically decaying
             W bosons and top quarks with large transverse momenta. A new
             type of jet input object, called a ‘unified flow object’
             is introduced which combines calorimeter- and
             inner-detector-based signals in order to achieve optimal
             performance across a wide kinematic range. Large-radius jet
             definitions are identified which significantly improve on
             the current ATLAS baseline definition, and their modelling
             is studied using pp collisions recorded by the ATLAS
             detector at s=13TeV during 2017.},
   Doi = {10.1140/epjc/s10052-021-09054-3},
   Key = {fds356048}
}

@article{fds346174,
   Author = {Mahesh, SH and Kushwaha, AS and Kotwal, A},
   Title = {Pandemic influenza: Experience in a flu OPD of a tertiary
             care hospital.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {70},
   Number = {1},
   Pages = {39-42},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.mjafi.2012.06.018},
   Abstract = {<h4>Background</h4>In April 2009, Mexican health authorities
             announced an outbreak of a novel H1N1 influenza virus, which
             subsequently caused a pandemic. The world is now moving into
             the post-pandemic period. The experience gained in handling
             this pandemic at various levels under different settings has
             provided us many lessons for the future.<h4>Objective</h4>To
             study the profile of various activities undertaken at flu
             screening centre as a response to pandemic influenza in a
             tertiary care hospital.<h4>Methods</h4>Record-based study
             conducted in a tertiary care hospital of Pune. Required data
             was collected from records of flu OPD, ward and local health
             authority and interviewing related staff. Study included
             data from October 2009 to October 2010.<h4>Results</h4>A
             total of 8020 people presenting with influenza like illness
             (ILI) were screened in the flu OPD under study. Out of
             these, only 388 (4.84%) met clinical criteria where throat
             samples were collected, out of which only 81 were found to
             be positive (20.88%). Total three fatalities (3.7%)
             occurred out of 81 who had tested positive. Most cases of
             flu were managed at home (76.54%) while only 19 (23.4%) lab
             confirmed cases of H1N1 required hospitalisation.<h4>Conclusion</h4>Majority
             of cases of H1N1 (2009) were managed at home. Early
             diagnosis, quick initiation of treatment, infection control
             measures, and good care at the hospital can effectively
             reduce morbidity and mortality in H1N1 pandemic.},
   Doi = {10.1016/j.mjafi.2012.06.018},
   Key = {fds346174}
}

@article{fds347496,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Dos
             Santos, SPA and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
             N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov,
             VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann,
             D and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
             TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
             S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and El Moursli and RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E},
   Title = {Performance of algorithms that reconstruct missing
             transverse momentum in [Formula: see text]= 8 TeV
             proton-proton collisions in the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {4},
   Pages = {241},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4780-2},
   Abstract = {The reconstruction and calibration algorithms used to
             calculate missing transverse momentum ([Formula: see text] )
             with the ATLAS detector exploit energy deposits in the
             calorimeter and tracks reconstructed in the inner detector
             as well as the muon spectrometer. Various strategies are
             used to suppress effects arising from additional
             proton-proton interactions, called pileup, concurrent with
             the hard-scatter processes. Tracking information is used to
             distinguish contributions from the pileup interactions using
             their vertex separation along the beam axis. The performance
             of the [Formula: see text] reconstruction algorithms,
             especially with respect to the amount of pileup, is
             evaluated using data collected in proton-proton collisions
             at a centre-of-mass energy of 8 [Formula: see text] during
             2012, and results are shown for a data sample corresponding
             to an integrated luminosity of [Formula: see text]. The
             simulation and modelling of [Formula: see text]  in events
             containing a <i>Z</i> boson decaying to two charged leptons
             (electrons or muons) or a <i>W</i> boson decaying to a
             charged lepton and a neutrino are compared to data. The
             acceptance for different event topologies, with and without
             high transverse momentum neutrinos, is shown for a range of
             threshold criteria for [Formula: see text] , and estimates
             of the systematic uncertainties in the [Formula: see text]
              measurements are presented.},
   Doi = {10.1140/epjc/s10052-017-4780-2},
   Key = {fds347496}
}

@article{fds315920,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Performance of b-jet identification in the ATLAS
             experiment},
   Journal = {Journal of Instrumentation},
   Volume = {11},
   Number = {4},
   Pages = {P04008-P04008},
   Publisher = {IOP Publishing},
   Year = {2016},
   Month = {April},
   url = {http://dx.doi.org/10.1088/1748-0221/11/04/P04008},
   Abstract = {The identification of jets containing b hadrons is important
             for the physics programme of the ATLAS experiment at the
             Large Hadron Collider. Several algorithms to identify jets
             containing b hadrons are described, ranging from those based
             on the reconstruction of an inclusive secondary vertex or
             the presence of tracks with large impact parameters to
             combined tagging algorithms making use of multi-variate
             discriminants. An independent b-tagging algorithm based on
             the reconstruction of muons inside jets as well as the
             b-tagging algorithm used in the online trigger are also
             presented. The b-jet tagging efficiency, the c-jet tagging
             efficiency and the mistag rate for light flavour jets in
             data have been measured with a number of complementary
             methods. The calibration results are presented as scale
             factors defined as the ratio of the efficiency (or mistag
             rate) in data to that in simulation. In the case of b jets,
             where more than one calibration method exists, the results
             from the various analyses have been combined taking into
             account the statistical correlation as well as the
             correlation of the sources of systematic
             uncertainty.},
   Doi = {10.1088/1748-0221/11/04/P04008},
   Key = {fds315920}
}

@article{fds356551,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Araque, JP and Ferraz, VA and Pereira,
             RA},
   Title = {Performance of electron and photon triggers in ATLAS during
             LHC Run 2},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {1},
   Year = {2020},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7500-2},
   Abstract = {Electron and photon triggers covering transverse energies
             from 5 GeV to several TeV are essential for the ATLAS
             experiment to record signals for a wide variety of physics:
             from Standard Model processes to searches for new phenomena
             in both proton–proton and heavy-ion collisions. To cope
             with a fourfold increase of peak LHC luminosity from 2015 to
             2018 (Run 2), to 2.1×1034cm-2s-1, and a similar increase in
             the number of interactions per beam-crossing to about 60,
             trigger algorithms and selections were optimised to control
             the rates while retaining a high efficiency for physics
             analyses. For proton–proton collisions, the
             single-electron trigger efficiency relative to a
             single-electron offline selection is at least 75% for an
             offline electron of 31 GeV, and rises to 96% at 60 GeV;
             the trigger efficiency of a 25 GeV leg of the primary
             diphoton trigger relative to a tight offline photon
             selection is more than 96% for an offline photon of 30 GeV.
             For heavy-ion collisions, the primary electron and photon
             trigger efficiencies relative to the corresponding standard
             offline selections are at least 84% and 95%, respectively,
             at 5 GeV above the corresponding trigger
             threshold.},
   Doi = {10.1140/epjc/s10052-019-7500-2},
   Key = {fds356551}
}

@article{fds307576,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
   Title = {Performance of jet substructure techniques for large-R jets
             in proton-proton collisions at √s=7 TeV using the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2013)076},
   Abstract = {This paper presents the application of a variety of
             techniques to study jet substructure. The performance of
             various modified jet algorithms, or jet grooming techniques,
             for several jet types and event topologies is investigated
             for jets with transverse momentum larger than 300 GeV.
             Properties of jets subjected to the mass-drop filtering,
             trimming, and pruning algorithms are found to have a reduced
             sensitivity to multiple proton-proton interactions, are more
             stable at high luminosity and improve the physics potential
             of searches for heavy boosted objects. Studies of the
             expected discrimination power of jet mass and jet
             substructure observables in searches for new physics are
             also presented. Event samples enriched in boosted W and Z
             bosons and top-quark pairs are used to study both the
             individual jet invariant mass scales and the efficacy of
             algorithms to tag boosted hadronic objects. The analyses
             presented use the full 2011 ATLAS dataset, corresponding to
             an integrated luminosity of 4.7 ± 0.1 fb-1 from
             proton-proton collisions produced by the Large Hadron
             Collider at a centre-of-mass energy of √s=7 TeV. [Figure
             not available: see fulltext.] © 2013 Cern for the benefit
             of the ATLAS collaboration.},
   Doi = {10.1007/JHEP09(2013)076},
   Key = {fds307576}
}

@article{fds307717,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, J and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D},
   Title = {Performance of missing transverse momentum reconstruction in
             proton-proton collisions at√s = 7 TeV with
             atlas},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {1},
   Pages = {1-35},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1844-6},
   Abstract = {The measurement of missing transverse momentum in the ATLAS
             detector, described in this paper, makes use of the full
             event reconstruction and a calibration based on
             reconstructed physics objects. The performance of the
             missing transverse momentum reconstruction is evaluated
             using data collected in pp collisions at a centre-of-mass
             energy of 7 TeV in 2010. Minimum bias events and events with
             jets of hadrons are used from data samples corresponding to
             an integrated luminosity of about 0.3 nb1 and 600 nb1
             respectively, together with events containing a Z boson
             decaying to two leptons (electrons or muons) or aW boson
             decaying to a lepton (electron or muon) and a neutrino, from
             a data sample corresponding to an integrated luminosity of
             about 36 pb1. An estimate of the systematic uncertainty on
             the missing transverse momentum scale is presented. © CERN
             for the benefit of the ATLAS collaboration
             2011.},
   Doi = {10.1140/epjc/s10052-011-1844-6},
   Key = {fds307717}
}

@article{fds347482,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson,
             TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
             H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee,
             S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
             AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov,
             G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini,
             D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks,
             T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina,
             E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioară, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Colasurdo,
             L},
   Title = {Performance of missing transverse momentum reconstruction
             with the ATLAS detector using proton-proton collisions at s
             = 13 TeV.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {11},
   Pages = {903},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-6288-9},
   Abstract = {The performance of the missing transverse momentum ( E T
             miss ) reconstruction with the ATLAS detector is evaluated
             using data collected in proton-proton collisions at the LHC
             at a centre-of-mass energy of 13 TeV in 2015. To
             reconstruct E T miss , fully calibrated electrons, muons,
             photons, hadronically decaying τ -leptons , and jets
             reconstructed from calorimeter energy deposits and
             charged-particle tracks are used. These are combined with
             the soft hadronic activity measured by reconstructed
             charged-particle tracks not associated with the hard
             objects. Possible double counting of contributions from
             reconstructed charged-particle tracks from the inner
             detector, energy deposits in the calorimeter, and
             reconstructed muons from the muon spectrometer is avoided by
             applying a signal ambiguity resolution procedure which
             rejects already used signals when combining the various E T
             miss contributions. The individual terms as well as the
             overall reconstructed E T miss are evaluated with various
             performance metrics for scale (linearity), resolution, and
             sensitivity to the data-taking conditions. The method
             developed to determine the systematic uncertainties of the E
             T miss scale and resolution is discussed. Results are shown
             based on the full 2015 data sample corresponding to an
             integrated luminosity of 3.2 fb - 1 .},
   Doi = {10.1140/epjc/s10052-018-6288-9},
   Key = {fds347482}
}

@article{fds321076,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa,
             M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton,
             AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates,
             RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer,
             F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin,
             PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker,
             M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
             A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella,
             G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
             JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford,
             L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock,
             I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Brown, J and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret,
             MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini,
             I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo,
             F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Barajas, CAC and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and El Moursli and RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G},
   Title = {Performance of pile-up mitigation techniques for jets in
             [Formula: see text] collisions at [Formula: see text] TeV
             using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {11},
   Pages = {581},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4395-z},
   Abstract = {The large rate of multiple simultaneous proton-proton
             interactions, or pile-up, generated by the Large Hadron
             Collider in Run 1 required the development of many new
             techniques to mitigate the adverse effects of these
             conditions. This paper describes the methods employed in the
             ATLAS experiment to correct for the impact of pile-up on jet
             energy and jet shapes, and for the presence of spurious
             additional jets, with a primary focus on the large
             20.3 [Formula: see text] data sample collected at a
             centre-of-mass energy of [Formula: see text]. The energy
             correction techniques that incorporate sophisticated
             estimates of the average pile-up energy density and tracking
             information are presented. Jet-to-vertex association
             techniques are discussed and projections of performance for
             the future are considered. Lastly, the extension of these
             techniques to mitigate the effect of pile-up on jet shapes
             using subtraction and grooming procedures is
             presented.},
   Doi = {10.1140/epjc/s10052-016-4395-z},
   Key = {fds321076}
}

@article{fds361307,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
             BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
             MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei,
             D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce,
             ATH and Arguin, JF and Argyropoulos, S},
   Title = {Performance of the ATLAS Level-1 topological trigger in
             Run 2},
   Journal = {European Physical Journal C},
   Volume = {82},
   Number = {1},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2022},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09807-0},
   Abstract = {During LHC Run 2 (2015–2018) the ATLAS Level-1
             topological trigger allowed efficient data-taking by the
             ATLAS experiment at luminosities up to 2.1× 1034 cm- 2s-
             1, which exceeds the design value by a factor of two. The
             system was installed in 2016 and operated in 2017 and 2018.
             It uses Field Programmable Gate Array processors to select
             interesting events by placing kinematic and angular
             requirements on electromagnetic clusters, jets, τ-leptons,
             muons and the missing transverse energy. It allowed to
             significantly improve the background event rejection and
             signal event acceptance, in particular for Higgs and
             B-physics processes.},
   Doi = {10.1140/epjc/s10052-021-09807-0},
   Key = {fds361307}
}

@article{fds310315,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
             O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
             V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Performance of the ATLAS muon trigger in pp collisions at
             [Formula: see text] TeV.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {3},
   Pages = {120},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3325-9},
   Abstract = {The performance of the ATLAS muon trigger system is
             evaluated with proton-proton collision data collected in
             2012 at the Large Hadron Collider at a centre-of-mass energy
             of 8 TeV. It is primarily evaluated using events containing
             a pair of muons from the decay of [Formula: see text]
             bosons. The efficiency of the single-muon trigger is
             measured for muons with transverse momentum [Formula: see
             text] GeV, with a statistical uncertainty of less than
             0.01 % and a systematic uncertainty of 0.6 %. The
             [Formula: see text] range for efficiency determination is
             extended by using muons from decays of [Formula: see text]
             mesons, [Formula: see text] bosons, and top quarks. The muon
             trigger shows highly uniform and stable performance. The
             performance is compared to the prediction of a detailed
             simulation.},
   Doi = {10.1140/epjc/s10052-015-3325-9},
   Key = {fds310315}
}

@article{fds354098,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso,
             S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Ferraz, VA and Pereira,
             RA},
   Title = {Performance of the ATLAS muon triggers in Run
             2},
   Journal = {Journal of Instrumentation},
   Volume = {15},
   Number = {9},
   Year = {2020},
   Month = {September},
   url = {http://dx.doi.org/10.1088/1748-0221/15/09/P09015},
   Abstract = {The performance of the ATLAS muon trigger system is
             evaluated with proton-proton (pp) and heavy-ion (HI)
             collision data collected in Run 2 during 2015-2018 at the
             Large Hadron Collider. It is primarily evaluated using
             events containing a pair of muons from the decay of Z bosons
             to cover the intermediate momentum range between 26 GeV and
             100 GeV. Overall, the efficiency of the single-muon triggers
             is about 68% in the barrel region and 85% in the endcap
             region. The pT range for efficiency determination is
             extended by using muons from decays of Jψ mesons, W bosons,
             and top quarks. The performance in HI collision data is
             measured and shows good agreement with the results obtained
             in pp collisions. The muon trigger shows uniform and stable
             performance in good agreement with the prediction of a
             detailed simulation. Dedicated multi-muon triggers with
             kinematic selections provide the backbone to beauty,
             quarkonia, and low-mass physics studies. The design,
             evolution and performance of these triggers are discussed in
             detail.},
   Doi = {10.1088/1748-0221/15/09/P09015},
   Key = {fds354098}
}

@article{fds358687,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso,
             S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen,
             T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA},
   Title = {Performance of the ATLAS RPC detector and Level-1 muon
             barrel trigger at √s = 13 TeV},
   Journal = {Journal of Instrumentation},
   Volume = {16},
   Number = {7},
   Year = {2021},
   Month = {July},
   url = {http://dx.doi.org/10.1088/1748-0221/16/07/P07029},
   Abstract = {The ATLAS experiment at the Large Hadron Collider (LHC)
             employs a trigger system consisting of a first-level
             hardware trigger (L1) and a software-based high-level
             trigger. The L1 muon trigger system selects muon candidates,
             assigns them to the correct LHC bunch crossing and
             classifies them into one of six transverse-momentum
             threshold classes. The L1 muon trigger system uses
             resistive-plate chambers (RPCs) to generate the muon-induced
             trigger signals in the central (barrel) region of the ATLAS
             detector. The ATLAS RPCs are arranged in six concentric
             layers and operate in a toroidal magnetic field with a
             bending power of 1.5 to 5.5 Tm. The RPC detector consists of
             about 3700 gas volumes with a total surface area of more
             than 4000 m2. This paper reports on the performance of the
             RPC detector and L1 muon barrel trigger using 60.8 fb-1 of
             proton-proton collision data recorded by the ATLAS
             experiment in 2018 at a centre-of-mass energy of 13 TeV.
             Detector and trigger performance are studied using Z boson
             decays into a muon pair. Measurements of the RPC detector
             response, efficiency, and time resolution are reported.
             Measurements of the L1 muon barrel trigger efficiencies and
             rates are presented, along with measurements of the
             properties of the selected sample of muon candidates.
             Measurements of the RPC currents, counting rates and mean
             avalanche charge are performed using zero-bias collisions.
             Finally, RPC detector response and efficiency are studied at
             different high voltage and front-end discriminator threshold
             settings in order to extrapolate detector response to the
             higher luminosity expected for the High Luminosity
             LHC.},
   Doi = {10.1088/1748-0221/16/07/P07029},
   Key = {fds358687}
}

@article{fds347511,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
             Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
             TJ and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Performance of the ATLAS track reconstruction algorithms in
             dense environments in LHC Run 2.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {10},
   Pages = {673},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5225-7},
   Abstract = {With the increase in energy of the Large Hadron Collider to
             a centre-of-mass energy of 13 [Formula: see text] for Run
             2, events with dense environments, such as in the cores of
             high-energy jets, became a focus for new physics searches as
             well as measurements of the Standard Model. These
             environments are characterized by charged-particle
             separations of the order of the tracking detectors sensor
             granularity. Basic track quantities are compared between
             3.2 fb[Formula: see text] of data collected by the ATLAS
             experiment and simulation of proton-proton collisions
             producing high-transverse-momentum jets at a centre-of-mass
             energy of 13 [Formula: see text]. The impact of
             charged-particle separations and multiplicities on the track
             reconstruction performance is discussed. The track
             reconstruction efficiency in the cores of jets with
             transverse momenta between 200 and 1600 [Formula: see text]
             is quantified using a novel, data-driven, method. The method
             uses the energy loss, [Formula: see text], to identify pixel
             clusters originating from two charged particles. Of the
             charged particles creating these clusters, the measured
             fraction that fail to be reconstructed is [Formula: see
             text] and [Formula: see text] for jet transverse momenta of
             200-400 [Formula: see text] and 1400-1600 [Formula: see
             text], respectively.},
   Doi = {10.1140/epjc/s10052-017-5225-7},
   Key = {fds347511}
}

@article{fds356751,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
             M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Verzini, MJA and Aleksa,
             M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Santos,
             SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Armitage, LJ},
   Title = {Performance of the ATLAS Transition Radiation Tracker in Run
             1 of the LHC: Tracker properties},
   Journal = {Journal of Instrumentation},
   Volume = {12},
   Number = {5},
   Year = {2017},
   Month = {May},
   url = {http://dx.doi.org/10.1088/1748-0221/12/05/P05002},
   Abstract = {The tracking performance parameters of the ATLAS Transition
             Radiation Tracker (TRT) as part of the ATLAS inner detector
             are described in this paper for different data-taking
             conditions in proton-proton, proton-lead and lead-lead
             collisions at the Large Hadron Collider (LHC). The
             performance is studied using data collected during the first
             period of LHC operation (Run 1) and is compared with Monte
             Carlo simulations. The performance of the TRT, operating
             with two different gas mixtures (xenon-based and
             argon-based) and its dependence on the TRT occupancy is
             presented. These studies show that the tracking performance
             of the TRT is similar for the two gas mixtures and that a
             significant contribution to the particle momentum resolution
             is made by the TRT up to high particle densities.},
   Doi = {10.1088/1748-0221/12/05/P05002},
   Key = {fds356751}
}

@article{fds307718,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Performance of the ATLAS trigger system in
             2010},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {1},
   Pages = {1-61},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1849-1},
   Abstract = {Proton-proton collisions at √S = 7 TeV and heavy ion
             collisions at √SNN = 2.76 TeV were produced by the LHC and
             recorded using the ATLAS experiment's trigger system in
             2010. The LHC is designed with a maximum bunch crossing rate
             of 40 MHz and the ATLAS trigger system is designed to record
             approximately 200 of these per second. The trigger system
             selects events by rapidly identifying signatures of muon,
             electron, photon, tau lepton, jet, and B meson candidates,
             as well as using global event signatures, such as missing
             transverse energy. An overview of the ATLAS trigger system,
             the evolution of the system during 2010 and the performance
             of the trigger system components and selections based on the
             2010 collision data are shown. A brief outline of plans for
             the trigger system in 2011 is presented.},
   Doi = {10.1140/epjc/s10052-011-1849-1},
   Key = {fds307718}
}

@article{fds347501,
   Author = {Atlas Collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten,
             K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
             A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Bell,
             AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
             J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer,
             F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin,
             S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke,
             S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
             S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda,
             E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro,
             NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez
             Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
             S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL and Clark, MR},
   Title = {Performance of the ATLAS trigger system in
             2015.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {5},
   Pages = {317},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4852-3},
   Abstract = {During 2015 the ATLAS experiment recorded [Formula: see
             text] of proton-proton collision data at a centre-of-mass
             energy of [Formula: see text]. The ATLAS trigger system is a
             crucial component of the experiment, responsible for
             selecting events of interest at a recording rate of
             approximately 1 kHz from up to 40 MHz of collisions. This
             paper presents a short overview of the changes to the
             trigger and data acquisition systems during the first long
             shutdown of the LHC and shows the performance of the trigger
             system and its components based on the 2015 proton-proton
             collision data.},
   Doi = {10.1140/epjc/s10052-017-4852-3},
   Key = {fds347501}
}

@article{fds352491,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei,
             V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {Performance of the missing transverse momentum triggers for
             the ATLAS detector during Run-2 data taking},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {8},
   Year = {2020},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2020)080},
   Abstract = {The factor of four increase in the LHC luminosity, from 0.5
             × 1034 cm−2s−1 to 2.0 × 1034cm−2s−1, and the
             corresponding increase in pile-up collisions during the
             2015–2018 data-taking period, presented a challenge for
             the ATLAS trigger, particularly for those algorithms that
             select events with missing transverse momentum. The output
             data rate at fixed threshold typically increases
             exponentially with the number of pile-up collisions, so the
             legacy algorithms from previous LHC data-taking periods had
             to be tuned and new approaches developed to maintain the
             high trigger efficiency achieved in earlier operations. A
             study of the trigger performance and comparisons with
             simulations show that these changes resulted in event
             selection efficiencies of > 98% for this period, meeting and
             in some cases exceeding the performance of similar triggers
             in earlier run periods, while at the same time keeping the
             necessary bandwidth within acceptable limits. [Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP08(2020)080},
   Key = {fds352491}
}

@article{fds375850,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel,
             A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed,
             WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh,
             B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
             AA and Cardoso, MA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler,
             A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
             J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Tame, ZPA and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten,
             K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Gupta, DB and Balasubramanian, R and Baldin,
             EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas,
             WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits,
             M-S and Barklow, T and Baron, P and Moreno, DAB and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Navarro, LB and Barreiro, F and da
             Costa, JBG and Barron, U and Teixeira, MGB and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Hurrell, LTB and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
             K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
             L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Kuutmann, EB and Berger, N and Bergmann, B and Beringer, J and Bernardi,
             G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta,
             P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
             V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Sola, JDB and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
             R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and de Renstrom, PAB and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
             CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Vazquez, CJB and Buzykaev, AR and Cabras, G and Urbán, SC and Cadamuro,
             L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace,
             N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Toro, RC and Camarda, S and Munoz, DC and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Bret, MC and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
             JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Argos, FC and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Garcia, LC and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini,
             G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
             Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and El Moursli and RC and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
             J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
             A},
   Title = {Performance of the reconstruction of large impact parameter
             tracks in the inner detector of ATLAS},
   Journal = {The European Physical Journal C},
   Volume = {83},
   Number = {11},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2023},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-12024-6},
   Abstract = {<jats:title>Abstract</jats:title><jats:p>Searches for
             long-lived particles (LLPs) are among the most promising
             avenues for discovering physics beyond the Standard Model at
             the Large Hadron Collider (LHC). However, displaced
             signatures are notoriously difficult to identify due to
             their ability to evade standard object reconstruction
             strategies. In particular, the ATLAS track reconstruction
             applies strict pointing requirements which limit sensitivity
             to charged particles originating far from the primary
             interaction point. To recover efficiency for LLPs decaying
             within the tracking detector volume, the ATLAS Collaboration
             employs a dedicated large-radius tracking (LRT) pass with
             loosened pointing requirements. During Run 2 of the LHC, the
             LRT implementation produced many incorrectly reconstructed
             tracks and was therefore only deployed in small subsets of
             events. In preparation for LHC Run 3, ATLAS has
             significantly improved both standard and large-radius track
             reconstruction performance, allowing for LRT to run in all
             events. This development greatly expands the potential
             phase-space of LLP searches and streamlines LLP analysis
             workflows. This paper will highlight the above achievement
             and report on the readiness of the ATLAS detector for
             track-based LLP searches in Run 3.</jats:p>},
   Doi = {10.1140/epjc/s10052-023-12024-6},
   Key = {fds375850}
}

@article{fds354096,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {Performance of the upgraded PreProcessor of the ATLAS
             Level-1 Calorimeter Trigger},
   Journal = {Journal of Instrumentation},
   Volume = {15},
   Number = {11},
   Year = {2020},
   Month = {November},
   url = {http://dx.doi.org/10.1088/1748-0221/15/11/P11016},
   Abstract = {The PreProcessor of the ATLAS Level-1 Calorimeter Trigger
             prepares the analogue trigger signals sent from the ATLAS
             calorimeters by digitising, synchronising, and calibrating
             them to reconstruct transverse energy deposits, which are
             then used in further processing to identify event features.
             During the first long shutdown of the LHC from 2013 to 2014,
             the central components of the PreProcessor, the Multichip
             Modules, were replaced by upgraded versions that feature
             modern ADC and FPGA technology to ensure optimal performance
             in the high pile-up environment of LHC Run 2. This paper
             describes the features of the new Multichip Modules along
             with the improvements to the signal processing
             achieved.},
   Doi = {10.1088/1748-0221/15/11/P11016},
   Key = {fds354096}
}

@article{fds356600,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos, SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Pozo, JAA and Aperio Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz, V and Araujo Pereira, R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {Performance of top-quark and W -boson tagging with ATLAS in
             Run 2 of the LHC},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {5},
   Year = {2019},
   Month = {May},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-6847-8},
   Abstract = {The performance of identification algorithms (“taggers”)
             for hadronically decaying top quarks and W bosons in pp
             collisions at s = 13 TeV recorded by the ATLAS experiment
             at the Large Hadron Collider is presented. A set of
             techniques based on jet shape observables are studied to
             determine a set of optimal cut-based taggers for use in
             physics analyses. The studies are extended to assess the
             utility of combinations of substructure observables as a
             multivariate tagger using boosted decision trees or deep
             neural networks in comparison with taggers based on
             two-variable combinations. In addition, for highly boosted
             top-quark tagging, a deep neural network based on jet
             constituent inputs as well as a re-optimisation of the
             shower deconstruction technique is presented. The
             performance of these taggers is studied in data collected
             during 2015 and 2016 corresponding to 36.1 fb - 1 for the
             tt¯ and γ+ jet and 36.7 fb - 1 for the dijet event
             topologies.},
   Doi = {10.1140/epjc/s10052-019-6847-8},
   Key = {fds356600}
}

@article{fds361714,
   Author = {Golling, T and Hance, M and Harris, P and Mangano, ML and McCullough, M and Moortgat, F and Schwaller, P and Torre, R and Agrawal, P and Alves, DSM and Antusch, S and Arbey, A and Auerbach, B and Bambhaniya, G and Battaglia,
             M and Bauer, M and Dev, PSB and Boveia, A and Bramante, J and Buchmueller,
             O and Buschmann, M and Chakrabortty, J and Chala, M and Chekanov, S and Chen, C-Y and Cheng, H-C and Cirelli, M and Citron, M and Cohen, T and Craig, N and Curtin, D and D'Agnolo, RT and Doglioni, C and Dror, JA and Pree, TD and Dylewsky, D and Ellis, J and Ellis, SAR and Essig, R and Fan,
             JJ and Farina, M and Feng, JL and Fox, PJ and Galloway, J and Giudice, G and Gluza, J and Gori, S and Guha, S and Hahn, K and Han, T and Helsens, C and Henriques, A and Iwamoto, S and Jelinski, T and Jung, S and Kahlhoefer,
             F and Khoze, VV and Kim, D and Kopp, J and Kotwal, A and Kraemer, M and Lindert, JM and Liu, J and Lou, HK and Love, J and Low, M and Machado, PAN and Mahmoudi, F and Marrouche, J and Martin, A and Mohan, K and Mohapatra,
             RN and Nardini, G and Olive, KA and Ostdiek, B and Panico, G and Plehn, T and Proudfoot, J and Qian, Z and Reece, M and Rizzo, T and Roskas, C and Ruderman, J and Ruiz, R and Sala, F and Salvioni, E and Saraswat, P and Schell, T and Schmidt-Hoberg, K and Serra, J and Shadmi, Y and Shelton,
             J and Solans, C and Spannowsky, M and Srivastava, T and Stolarski, D and Szafron, R and Taoso, M and Tarem, S and Thalapillil, A and Thamm, A and Tsai, Y and Verhaaren, C and Vignaroli, N and Walsh, JR and Wang, LT and Weiland, C and Wells, J and Williams, C and Wulzer, A and Xue, W and Yu, F and Zheng, B and Zheng, J},
   Title = {Physics at a 100 TeV pp collider: beyond the Standard Model
             phenomena},
   Year = {2016},
   Month = {June},
   Abstract = {This report summarises the physics opportunities in the
             search and study of physics beyond the Standard Model at a
             100 TeV pp collider.},
   Key = {fds361714}
}

@article{fds212567,
   Author = {A.V. Kotwal and ATLAS Collaboration},
   Title = {Physics at a High-Luminosity LHC with ATLAS},
   Journal = {ATL-PHYS-PUB-2012-004},
   Year = {2012},
   Month = {October},
   Key = {fds212567}
}

@article{fds362581,
   Author = {Baur, U and Brock, R and Parsons, J and Albrow, M and Denisov, D and Han,
             T and Kotwal, A and Olness, F and Qian, J and Belyaev,
             S},
   Title = {Physics at Future Hadron Colliders},
   Journal = {eConf C},
   Volume = {010630},
   Pages = {E4001},
   Year = {2002},
   Month = {January},
   Abstract = {We discuss the physics opportunities and detector challenges
             at future hadron colliders. As guidelines for energies and
             luminosities we use the proposed luminosity and/or energy
             upgrade of the LHC (SLHC), and the Fermilab design of a Very
             Large Hadron Collider (VLHC). We illustrate the physics
             capabilities of future hadron colliders for a variety of new
             physics scenarios (supersymmetry, strong electroweak
             symmetry breaking, new gauge bosons, compositeness and extra
             dimensions). We also investigate the prospects of doing
             precision Higgs physics studies at such a machine, and list
             selected Standard Model physics rates.},
   Key = {fds362581}
}

@article{fds352598,
   Author = {Chekanov, SV and Kotwal, AV and Yeh, CH and Yu, SS},
   Title = {Physics potential of timing layers in future collider
             detectors},
   Journal = {Journal of Instrumentation},
   Volume = {15},
   Number = {9},
   Year = {2020},
   Month = {September},
   url = {http://dx.doi.org/10.1088/1748-0221/15/09/P09021},
   Abstract = {The physics potential of timing layers with a few tens of
             pico-second resolution in the calorimeters of future
             collider detectors is explored. These studies show how such
             layers can be used for particle identification and
             illustrate the potential for detecting new event signatures
             originating from physics beyond the standard
             model.},
   Doi = {10.1088/1748-0221/15/09/P09021},
   Key = {fds352598}
}

@article{fds308254,
   Author = {Laymon, CM and Amos, W and Burlein, MG and Fortune, HT and Ekenberg, T and Kotwal, A and O'Donnell, JM and Silk, JD and Zumbro, JD and Morris, CL and Seestrom, SJ and Dhuga, KS and Garnett, R and Rawool-Sullivan, MW and Moore, CF and Morris, SL and Watson, DL},
   Title = {Pion elastic and inelastic 21+ scattering on 58,60,62,64Ni
             at T pi =180 MeV.},
   Journal = {Physical review. C, Nuclear physics},
   Volume = {53},
   Number = {3},
   Pages = {1167-1172},
   Year = {1996},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevc.53.1167},
   Abstract = {Angular distributions for π+ and π- elastic and inelastic
             scattering from the Z=28 closed-proton-shell nuclei
             58,50,62,64Ni have been measured at an incident pion kinetic
             energy of 180 MeV. Values for the neutron and proton matrix
             elements for the transition to the Jπ=2+1 state have been
             extracted using the distorted wave impulse approximation in
             which the π+ and π- data were fitted simultaneously and
             the neutron and proton vibrational transition strengths were
             treated as free parameters. While all transitions are
             predominantly collective, extracted values of M n|Mp
             indicate increasing collectivity as a function of neutron
             number and are consistent with the collective limit of N|Z
             for 64Ni.},
   Doi = {10.1103/physrevc.53.1167},
   Key = {fds308254}
}

@article{fds308259,
   Author = {Burlein, M and Fortune, HT and Amos, WM and Ekenberg, TL and Kotwal, A and Kutt, PH and O'Donnell, JM and Silk, JD and Boyer, B and Fuentes, A and Johnson, K and Moore, CF and Yoo, SH and Mordechai, S and Morris, CL and Zumbro, JD and Watson, DL and Dhuga, KS},
   Title = {Pion inelastic scattering to low-lying positive-parity
             states in 20Ne.},
   Journal = {Physical review. C, Nuclear physics},
   Volume = {51},
   Number = {1},
   Pages = {88-97},
   Year = {1995},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevc.51.88},
   Abstract = {We have measured pion inelastic scattering from Ne20 with
             180 MeV π+ and π- at 12°and from 15°to 90°in 5°steps
             and with 120 MeV π+ from 15°to 90°in 5°steps. We report
             here on states in the first four Kπ=0+ bands, including the
             6.73MeV 0+ and the 8.78-MeV 6+ levels. Coupled-channels
             processes are shown to be important for many states. © 1995
             The American Physical Society.},
   Doi = {10.1103/physrevc.51.88},
   Key = {fds308259}
}

@article{fds308261,
   Author = {Burlein, M and Fortune, HT and Amos, WM and Ekenberg, TL and Kotwal, A and Kutt, PH and O'Donnell, JM and Silk, JD and Boyer, B and Fuentes, A and Johnson, K and Moore, CF and Yoo, SH and Mordechai, S and Morris, CL and Zumbro, JD and Watson, DL and Dhuga, KS},
   Title = {Pion inelastic scattering to the low-lying broad 2+ in
             20Ne.},
   Journal = {Physical review. C, Nuclear physics},
   Volume = {40},
   Number = {2},
   Pages = {785-789},
   Year = {1989},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevc.40.785},
   Abstract = {We have observed the broad 2+ member of the K=04+ band of
             Ne20 with the Ne20() reaction at T=120 and 180 MeV and with
             Ne20() at T=180 MeV. We find an excitation energy of
             9.000.18 MeV and a width of 0.8 MeV. The B(E2) is determined
             to be approximately 25 to 35 e2fm4. © 1989 The American
             Physical Society.},
   Doi = {10.1103/physrevc.40.785},
   Key = {fds308261}
}

@article{fds308260,
   Author = {Watson, DL and Gilman, R and Morris, CL and Zumbro, JD and Mordechai, S and Burlein, M and Odonnell, JM and Fortune, HT and Kotwal, A and Puttz, J and Silk, JD and McDonald, JS and Moore, CF and Williams, AL and Yoo,
             SY},
   Title = {Pion-induced double charge exchange on C12, Mg24, S32, and
             Ca40},
   Journal = {Physical Review C},
   Volume = {43},
   Number = {3},
   Pages = {1318-1320},
   Publisher = {American Physical Society (APS)},
   Year = {1991},
   url = {http://dx.doi.org/10.1103/PhysRevC.43.1318},
   Abstract = {Angular distributions for pion-induced double-charge-exchange
             (DCX) reaction have been measured at 164 MeV on the T=0
             target nuclei C12, Mg24, S32, and Ca40. The data are
             compared to calculations using the nucleon interaction model
             with realistic wave functions and NN and NN form factors
             deduced from fits to previously published DCX data on O16.
             The calculations reproduce the general shape of the angular
             distributions and the absolute magnitude of the cross
             sections to within a factor of two. © 1991 The American
             Physical Society.},
   Doi = {10.1103/PhysRevC.43.1318},
   Key = {fds308260}
}

@article{fds362573,
   Author = {Brock, R and Peskin, ME and Agashe, K and Artuso, M and Campbell, J and Dawson, S and Erbacher, R and Gerber, C and Gershtein, Y and Gritsan, A and Hatakeyama, K and Huston, J and Kotwal, A and Logan, H and Luty, M and Melnikov, K and Narain, M and Papucci, M and Petriello, F and Prell, S and Qian, J and Schwienhorst, R and Tully, C and Kooten, RV and Wackeroth,
             D and Wang, L and Whiteson, D},
   Title = {Planning the Future of U.S. Particle Physics (Snowmass
             2013): Chapter 3: Energy Frontier},
   Year = {2014},
   Month = {January},
   Abstract = {These reports present the results of the 2013 Community
             Summer Study of the APS Division of Particles and Fields
             ("Snowmass 2013") on the future program of particle physics
             in the U.S. Chapter 3, on the Energy Frontier, discusses the
             program of research with high-energy colliders. This area
             includes experiments on the Higgs boson, the electroweak and
             strong interactions, and the top quark. It also encompasses
             direct searches for new particles and interactions at high
             energy.},
   Key = {fds362573}
}

@article{fds344669,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi,
             A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Behari,
             S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas,
             J and Culbertson, R and Cully, JC and Daronco, S and Datta, M and D'Auria,
             S and Davies, T and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher,
             A and Lentdecker, GD and Lorenzo, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Dörr, C and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes,
             D and Giagu, S and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg,
             C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel,
             U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraan, AC and Kraus,
             J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
             C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
             J and Lysak, R and Lytken, E and MacK, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
             A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moon, CS and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
             G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn,
             F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle,
             T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy,
             L and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard,
             PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber,
             I and Sidoti, A},
   Title = {Polarizations of J/ψ and ψ(2S) mesons produced in pp̄
             collisions at s=1.96TeV},
   Journal = {Physical Review Letters},
   Volume = {99},
   Number = {13},
   Pages = {132001},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.99.132001},
   Abstract = {We have measured the polarizations of J/ψ and ψ(2S) mesons
             as functions of their transverse momentum pT when they are
             produced promptly in the rapidity range |y|&lt;0.6 with pT
             5GeV/c. The analysis is performed using a data sample with
             an integrated luminosity of about 800pb-1 collected by the
             CDF II detector. For both vector mesons, we find that the
             polarizations become increasingly longitudinal as pT
             increases from 5 to 30GeV/c. These results are compared to
             the predictions of nonrelativistic quantum chromodynamics
             and other contemporary models. The effective polarizations
             of J/ψ and ψ(2S) mesons from B-hadron decays are also
             reported. © 2007 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.99.132001},
   Key = {fds344669}
}

@article{fds308049,
   Author = {Abulencia, and A, and others},
   Title = {Precise measurement of the top quark mass in the lepton+jets
             topology at CDF II},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {18},
   Pages = {182002},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.99.182002},
   Abstract = {We present a measurement of the mass of the top quark from
             proton-antiproton collisions recorded at the CDF experiment
             in Run II of the Fermilab Tevatron. We analyze events from
             the single lepton plus jets final state (t[overline
             t]-->W+bW-[overline b]-->lnubq[overline q][prime][overline
             b]). The top-quark mass is extracted using a direct
             calculation of the probability density that each event
             corresponds to the t[overline t] final state. The
             probability is a function of both the mass of the top quark
             and the energy scale of the calorimeter jets, which is
             constrained in situ by the hadronic W boson mass. Using 167
             events observed in 955 pb-1 of integrated luminosity, we
             achieve the single most precise measurement of the top-quark
             mass, 170.8$\pm$2.2(stat.)$\pm$1.4(syst.)
             GeV/c2.},
   Doi = {10.1103/physrevlett.99.182002},
   Key = {fds308049}
}

@article{fds307541,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Guimaraes Da Costa and J and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
             M and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith,
             D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
             DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
             B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A},
   Title = {Precise measurement of the W -boson mass with the Collider
             Detector at Fermilab},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {7},
   Pages = {072003},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.072003},
   Abstract = {We present a measurement of the W-boson mass, MW, using data
             corresponding to 2.2fb-1 of integrated luminosity collected
             in pp̄ collisions at s=1.96TeV with the CDF II detector at
             the Fermilab Tevatron. The selected sample of 470126 W→eν
             candidates and 624708 W→μν candidates yields the
             measurement MW=80387±12(stat)±15(syst)=80387±19MeV/c2.
             This is the most precise single measurement of the W-boson
             mass to date. © 2014 American Physical Society.},
   Doi = {10.1103/PhysRevD.89.072003},
   Key = {fds307541}
}

@article{fds307709,
   Author = {Kotwal, AV and Collaboration, CDF},
   Title = {Precise Measurement of the W-Boson Mass with the CDF II
             Detector},
   Journal = {Phys. Rev. Lett.},
   Volume = {108},
   Number = {15},
   Pages = {151803},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.108.151803},
   Abstract = {We have measured the W-boson mass M(W) using data
             corresponding to 2.2  fb(-1) of integrated luminosity
             collected in pp collisions at sqrt[s] = 1.96  TeV with
             the CDF II detector at the Fermilab Tevatron collider.
             Samples consisting of 470,126 W → eν candidates and
             624,708 W → μν candidates yield the measurement M(W) =
             80,387 ± 12(stat.) ± 15(syst.) = 80,387 ± 19  MeV/c2.
             This is the most precise measurement of the W-boson mass to
             date and significantly exceeds the precision of all previous
             measurements combined.},
   Doi = {10.1103/physrevlett.108.151803},
   Key = {fds307709}
}

@article{fds347503,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
             H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
             A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti,
             M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
             J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho,
             J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
             Alberich, L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan,
             SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C},
   Title = {Precision measurement and interpretation of inclusive W+ ,
             W- and Z/γ∗ production cross sections with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {6},
   Pages = {367},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4911-9},
   Abstract = {High-precision measurements by the ATLAS Collaboration are
             presented of inclusive W+→ℓ+ν , W-→ℓ-ν¯ and
             Z/γ∗→ℓℓ ( ℓ=e,μ ) Drell-Yan production cross
             sections at the LHC. The data were collected in
             proton-proton collisions at s=7TeV with an integrated
             luminosity of 4.6fb-1 . Differential W+ and W- cross
             sections are measured in a lepton pseudorapidity range
             |ηℓ|<2.5 . Differential Z/γ∗ cross sections are
             measured as a function of the absolute dilepton rapidity,
             for |yℓℓ|<3.6 , for three intervals of dilepton mass,
             mℓℓ , extending from 46 to 150GeV . The integrated and
             differential electron- and muon-channel cross sections are
             combined and compared to theoretical predictions using
             recent sets of parton distribution functions. The data,
             together with the final inclusive e±p scattering
             cross-section data from H1 and ZEUS, are interpreted in a
             next-to-next-to-leading-order QCD analysis, and a new set of
             parton distribution functions, ATLAS-epWZ16, is obtained.
             The ratio of strange-to-light sea-quark densities in the
             proton is determined more accurately than in previous
             determinations based on collider data only, and is
             established to be close to unity in the sensitivity range of
             the data. A new measurement of the CKM matrix element |Vcs|
             is also provided.},
   Doi = {10.1140/epjc/s10052-017-4911-9},
   Key = {fds347503}
}

@article{fds307939,
   Author = {Aaltonen, T and others},
   Title = {Precision Measurement of the Ξ(3872) Mass in J/ψ π
             + π- Decays},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {15},
   Pages = {152001},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.152001},
   Abstract = {We present an analysis of the mass of the X(3872)
             reconstructed via its decay to J/ψπ+π- using
             2.4  fb-1 of integrated luminosity from pp̅ collisions
             at sqrt[s]=1.96  TeV, collected with the CDF II detector
             at the Fermilab Tevatron. The possible existence of two
             nearby mass states is investigated. Within the limits of our
             experimental resolution the data are consistent with a
             single state, and having no evidence for two states we set
             upper limits on the mass difference between two hypothetical
             states for different assumed ratios of contributions to the
             observed peak. For equal contributions, the 95% confidence
             level upper limit on the mass difference is 3.6  MeV/c2.
             Under the single-state model the X(3872) mass is measured to
             be 3871.61 &plusmn; 0.16(stat) &plusmn; 0.19(syst)  MeV/c2,
             which is the most precise determination to
             date.},
   Doi = {10.1103/physrevlett.103.152001},
   Key = {fds307939}
}

@article{fds308072,
   Author = {Abulencia, and A, and others},
   Title = {Precision measurement of the top quark mass from dilepton
             events at CDF II},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {3},
   Pages = {031105},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.031105},
   Abstract = {We report a measurement of the top-quark mass, Mt, in the
             dilepton decay channel of t[overline t]-->b[script-l][prime]+nu[script-l][prime][overline
             b][script-l]-[overline nu ][script-l] using an integrated
             luminosity of 1.0 fb-1 of p[overline p] collisions collected
             with the CDF II detector. We apply a method that convolutes
             a leading-order matrix element with detector resolution
             functions to form event-by-event likelihoods; we have
             enhanced the leading-order description to describe the
             effects of initial-state radiation. The joint likelihood is
             the product of the likelihoods from 78 candidate events in
             this sample, which yields a measurement of
             Mt=164.5$\pm$3.9(stat.)$\pm$3.9(syst.) GeV/c2, the most
             precise measurement of Mt in the dilepton
             channel.},
   Doi = {10.1103/PhysRevD.75.031105},
   Key = {fds308072}
}

@article{fds140618,
   Author = {Ashutosh V. Kotwal and A. Abulencia et al. [CDF
             Collaboration]},
   Title = {Precision measurement of the top-quark mass from dilepton
             events at CDF II},
   Journal = {Physical Review D (Rapid Communication)},
   Volume = {75},
   Number = {031105},
   Year = {2007},
   Month = {February},
   url = {http://link.aps.org/abstract/PRD/v75/e031105},
   Keywords = {top • mass},
   Abstract = {We report a measurement of the top-quark mass, Mt, in the
             dilepton decay channel of t tbar-->b l nu + b l nu using an
             integrated luminosity of 1.0/fb of p-pbar collisions
             collected with the CDF II detector. We apply a method that
             convolutes a leading-order matrix element with detector
             resolution functions to form event-by-event likelihoods; we
             have enhanced the leading-order description to describe the
             effects of initial-state radiation. The joint likelihood is
             the product of the likelihoods from 78 candidate events in
             this sample, which yields a measurement of Mt = 164.5 +-
             3.9(stat.) +- 3.9(syst.) GeV/c^2, the most precise
             measurement of Mt in the dilepton channel.},
   Key = {fds140618}
}

@article{fds308104,
   Author = {Abulencia, and A, and others},
   Title = {Precision top quark mass measurement in the lepton + jets
             topology in p anti-p collisions at $\sqrt{s}=$
             1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {2},
   Pages = {022004},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.022004},
   Abstract = {We report two measurements of the top quark mass M_top using
             the CDF II detector at the Fermilab Tevatron in a 318 pb-1
             data sample observed in the lepton + jets final state. One
             method uses an event-based likelihood technique resulting in
             M_top = 173.2+2.6_-2.4 (stat.) +/- 3.2 (syst.) GeV/c2 or
             173.2+4.1_-40 GeV/c2. The second method reconstructs a top
             quark mass in each event using the measured invariant mass
             of the hadronically decaying W boson to constrain the jet
             energy scale to obtain a value for M_top of 173.5+3.7_-3.6
             (stat.) +/- 1.3 (syst.) GeV/c2 or 173.5+3.9_-3.8 GeV/c2. We
             take the latter, which is more precise, as our
             result.},
   Doi = {10.1103/physrevlett.96.022004},
   Key = {fds308104}
}

@article{fds307682,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Precision top-quark mass measurement at CDF.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {15},
   Pages = {152003},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.109.152003},
   Abstract = {We present a precision measurement of the top-quark mass
             using the full sample of Tevatron √s = 1.96 TeV
             proton-antiproton collisions collected by the CDF II
             detector, corresponding to an integrated luminosity of 8.7
             fb(-1). Using a sample of tt¯ candidate events decaying
             into the lepton+jets channel, we obtain distributions of the
             top-quark masses and the invariant mass of two jets from the
             W boson decays from data. We then compare these
             distributions to templates derived from signal and
             background samples to extract the top-quark mass and the
             energy scale of the calorimeter jets with in situ
             calibration. The likelihood fit of the templates from signal
             and background events to the data yields the single
             most-precise measurement of the top-quark mass,
             M(top)=172.85±0.71(stat)±0.85(syst) GeV/c(2).},
   Doi = {10.1103/physrevlett.109.152003},
   Key = {fds307682}
}

@article{fds346205,
   Author = {Tendulkar, RD and Chellman-Jeffers, M and Rybicki, LA and Rim, A and Kotwal, A and Macklis, R and Obi, BB},
   Title = {Preoperative breast magnetic resonance imaging in early
             breast cancer: implications for partial breast
             irradiation.},
   Journal = {Cancer},
   Volume = {115},
   Number = {8},
   Pages = {1621-1630},
   Year = {2009},
   Month = {April},
   url = {http://dx.doi.org/10.1002/cncr.24172},
   Abstract = {<h4>Background</h4>Accelerated partial breast irradiation
             (APBI) of patients with early breast cancer is being
             investigated on a multi-institutional protocol National
             Surgical Adjuvant Breast and Bowel Project (NSABP) B-39/RTOG
             0413. Breast magnetic resonance imaging (MRI) is more
             sensitive than mammography (MG) and may aid in selection of
             patients appropriate for PBI.<h4>Methods</h4>Patients with
             newly diagnosed breast cancer or ductal carcinoma in situ
             (DCIS) routinely undergo contrast-enhanced, bilateral breast
             MRI at the Cleveland Clinic. We retrospectively reviewed the
             medical records of all early-stage breast cancer patients
             who had a breast MRI, MG, and surgical pathology data at our
             institution between June of 2005 and December of 2006. Any
             suspicious lesions identified on MRI were further evaluated
             by targeted ultrasound +/- biopsy.<h4>Results</h4>A total of
             260 patients met eligibility criteria for NSABP B-39/RTOG
             0413 by MG, physical exam, and surgical pathology. The
             median age was 57 years. DCIS was present in 63 patients,
             and invasive breast cancer was found in 197 patients. MRI
             identified suspicious lesions in 35 ipsilateral breasts
             (13%) and in 16 contralateral breasts (6%). Mammographically
             occult, synchronous ipsilateral foci were found by MRI in 11
             patients (4.2%), and in the contralateral breast in 4
             patients (1.5%). By univariate analysis, lobular histology
             (infiltrating lobular carcinoma [ILC]), pathologic T2, and
             American Joint Committee on Cancer stage II were
             significantly associated with additional ipsilateral
             disease. Of patients with ILC histology, 18% had ipsilateral
             secondary cancers or DCIS, compared with 3% in the remainder
             of histologic subtypes (P = .004). No patient older than 70
             years had synchronous cancers or DCIS detected by
             MRI.<h4>Conclusions</h4>Breast MRI identified synchronous
             mammographically occult foci in 5.8% of early breast cancer
             patients who would otherwise be candidates for
             APBI.},
   Doi = {10.1002/cncr.24172},
   Key = {fds346205}
}

@article{fds346177,
   Author = {Kumar, P and Londhe, SM and Kotwal, A and Mitra, R},
   Title = {Prevalence of malocclusion and orthodontic treatment need in
             schoolchildren - An epidemiological study.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {69},
   Number = {4},
   Pages = {369-374},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.mjafi.2012.02.003},
   Abstract = {<h4>Background</h4>To ascertain the prevalence of
             malocclusion and orthodontic treatment need in
             schoolchildren dependent on armed forces personnel. To
             review the overall oral health using DMFT index and to
             evaluate any relation between increased DMFT index to
             existing orthodontic problems.<h4>Method</h4>Five schools
             were randomly selected among Army/KV/AF schools and a random
             sample of 1200 children aged 10-15 years old attending these
             schools dependant on armed forces personnel were selected. A
             survey form was filled up after the examination of children
             by the principal worker and need for orthodontic treatment
             was assessed using index for orthodontic treatment need
             (IOTN) and overall oral health status by DMFT index and
             totaled. Frontal intra oral photograph in centric occlusion
             were taken. Dental Health Component (DHC) of IOTN for all
             the patients was marked by one set of orthodontists. The
             most severe occlusal trait was identified by the examiner
             for any particular patient and the patient was then
             categorized according to this most severe trait. AC of the
             IOTN was assessed by second orthodontist, individual and a
             layperson.<h4>Results</h4>It was observed that prevalence of
             malocclusion in the sample was 53.7%. 32.8% (239 males & 154
             females) of samples are in need of orthodontic treatment.
             55.1% of samples shown no caries risk, 38.1% had moderate
             caries risk and 6.8% had high caries risk.<h4>Conclusion</h4>Significant
             percentage of the samples are in need for orthodontic
             treatment. There is significant relation between higher DMFT
             index and orthodontic treatment need. It was found that IOTN
             is a reliable and user-friendly index, which can be used for
             orthodontic surveys.},
   Doi = {10.1016/j.mjafi.2012.02.003},
   Key = {fds346177}
}

@booklet{Abbott98,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri,
             SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson,
             JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
             HT and Diesburg, M and di Loreto, G and Draper, P and Ducros, Y and Dudko,
             LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
             VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
             OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein,
             D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak,
             Y},
   Title = {Probing hard color-singlet exchange in pp̄ collisions at
             √s = 630 GeV and 1800 GeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {440},
   Number = {1-2},
   Pages = {189-202},
   Publisher = {Elsevier BV},
   Year = {1998},
   Month = {November},
   url = {http://dx.doi.org/10.1016/S0370-2693(98)01238-6},
   Abstract = {We present results on dijet production via hard
             color-singlet exchange in proton-antiproton collisions at
             √s = 630 GeV and 1800 GeV using the DØ detector. The
             fraction of dijet events produced via color-singlet exchange
             is measured as a function of jet transverse energy,
             separation in pseudorapidity between the two highest
             transverse energy jets, and proton-antiproton center-of-mass
             energy. The results are consistent with a color-singlet
             fraction that increases with an increasing fraction of
             quark-initiated processes and inconsistent with two-gluon
             models for the hard color-singlet. © 1998 Published by
             Elsevier Science B.V. All rights reserved.},
   Doi = {10.1016/S0370-2693(98)01238-6},
   Key = {Abbott98}
}

@article{fds321128,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
             M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
             C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biesuz,
             NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard,
             CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho
             Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman,
             JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
             S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
             K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
   Title = {Probing lepton flavour violation via neutrinoless [Formula:
             see text] decays with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {232},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4041-9},
   Abstract = {This article presents the sensitivity of the ATLAS
             experiment to the lepton-flavour-violating decays of
             [Formula: see text]. A method utilising the production of
             [Formula: see text] leptons via [Formula: see text] decays
             is used. This method is applied to the sample of
             20.3 fb[Formula: see text] of <i>pp</i> collision data at a
             centre-of-mass energy of 8 TeV collected by the ATLAS
             experiment at the LHC in 2012. No event is observed passing
             the selection criteria, and the observed (expected) upper
             limit on the [Formula: see text] lepton branching fraction
             into three muons, [Formula: see text], is [Formula: see
             text] ([Formula: see text]) at 90 % confidence
             level.},
   Doi = {10.1140/epjc/s10052-016-4041-9},
   Key = {fds321128}
}

@article{fds376062,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
             Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
             JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena,
             E},
   Title = {Probing the CP nature of the top–Higgs Yukawa coupling in
             tt¯H and tH events with H→bb¯ decays using the ATLAS
             detector at the LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {849},
   Year = {2024},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2024.138469},
   Abstract = {The CP properties of the coupling between the Higgs boson
             and the top quark are investigated using 139 fb−1 of
             proton–proton collision data recorded by the ATLAS
             experiment at the LHC at a centre-of-mass energy of s=13
             TeV. The CP structure of the top quark–Higgs boson Yukawa
             coupling is probed in events with a Higgs boson decaying
             into a pair of b-quarks and produced in association with
             either a pair of top quarks, tt¯H, or a single top quark,
             tH. Events containing one or two electrons or muons are used
             for the measurement. Multivariate techniques are used to
             select regions enriched in tt¯H and tH events, where
             dedicated CP-sensitive observables are exploited. In an
             extension of the Standard Model (SM) with a CP-odd admixture
             in the top–Higgs Yukawa coupling, the mixing angle between
             CP-even and CP-odd couplings is measured to be
             α=11−73∘∘+52∘, compatible with the SM prediction
             corresponding to α=0.},
   Doi = {10.1016/j.physletb.2024.138469},
   Key = {fds376062}
}

@article{fds347457,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
             Pereira, R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic, M and Bakalis,
             C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
             M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
             KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
             U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
             PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
             TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
             BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
             S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară,
             IA},
   Title = {Probing the Quantum Interference between Singly and Doubly
             Resonant Top-Quark Production in pp Collisions at
             sqrt[s]=13  TeV with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {121},
   Number = {15},
   Pages = {152002},
   Year = {2018},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.121.152002},
   Abstract = {This Letter presents a normalized differential cross-section
             measurement in a fiducial phase-space region where
             interference effects between top-quark pair production and
             associated production of a single top quark with a W boson
             and a b-quark are significant. Events with exactly two
             leptons (ee, μμ, or eμ) and two b-tagged jets that
             satisfy a multiparticle invariant mass requirement are
             selected from 36.1  fb^{-1} of proton-proton collision
             data taken at sqrt[s]=13  TeV with the ATLAS detector at
             the LHC in 2015 and 2016. The results are compared with
             predictions from simulations using various strategies for
             the interference. The standard prescriptions for
             interference modeling are significantly different from each
             other but are within 2σ of the data. State-of-the-art
             predictions that naturally incorporate interference effects
             provide the best description of the data in the measured
             region of phase space most sensitive to these effects. These
             results provide an important constraint on interference
             models and will guide future model development and
             tuning.},
   Doi = {10.1103/physrevlett.121.152002},
   Key = {fds347457}
}

@article{fds356756,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
             H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
             D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Probing the W tb vertex structure in t-channel
             single-top-quark production and decay in pp collisions at
             √s=8 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {4},
   Year = {2017},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2017)124},
   Abstract = {To probe the W tb vertex structure, top-quark and W -boson
             polarisation observables are measured from t-channel
             single-top-quark events produced in proton-proton collisions
             at a centre-of-mass energy of 8 TeV. The dataset corresponds
             to an integrated luminosity of 20.2 fb−1, recorded with
             the ATLAS detector at the LHC. Selected events contain one
             isolated electron or muon, large missing transverse momentum
             and exactly two jets, with one of them identified as likely
             to contain a b-hadron. Stringent selection requirements are
             applied to discriminate t-channel single-top-quark events
             from background. The polarisation observables are extracted
             from asymmetries in angular distributions measured with
             respect to spin quantisation axes appropriately chosen for
             the top quark and the W boson. The asymmetry measurements
             are performed at parton level by correcting the observed
             angular distributions for detector effects and hadronisation
             after subtracting the background contributions. The measured
             top-quark and W -boson polarisation values are in agreement
             with the Standard Model predictions. Limits on the imaginary
             part of the anomalous coupling gR are also set from
             model-independent measurements.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP04(2017)124},
   Key = {fds356756}
}

@article{fds310119,
   Author = {Kotwal, AV and Hays, C},
   Title = {Production and decay of spinning black holes at colliders
             and tests of black hole dynamics},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {66},
   Number = {11},
   Pages = {116005},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.66.116005},
   Abstract = {We analyze the angular momentum distribution of black holes
             produced in high energy collisions in space-times with extra
             spatial dimensions. We show that the black hole spin
             significantly affects the energy and angular spectra of
             Hawking radiation. Our results show the experimental
             sensitivity to the angular momentum distribution and provide
             tests of black hole production dynamics. © 2002 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.66.116005},
   Key = {fds310119}
}

@article{fds310397,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Production of KS0, K*(892) and φ0(1020) in minimum bias
             events and KS0 and Λ0 in jets in pp̄ collisions at
             √s=1.96 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.092005},
   Abstract = {We report measurements of the inclusive transverse momentum
             (pT) distribution of centrally produced KS0, K±(892), and
             φ0(1020) mesons up to pT=10 GeV/c in minimum bias events,
             and KS0 and Λ0 particles up to pT=20 GeV/c in jets with
             transverse energy between 25 and 160 GeV in pp̄ collisions.
             The data were taken with the CDF II detector at the Fermilab
             Tevatron at √s=1.96 TeV. We find that as pT increases, the
             pT slopes of the three mesons (KS0, K±, and φ) are
             similar. And using our previous Λ0 results from minimum
             bias events, we show that the ratio of Λ0 to KS0 as a
             function of pT in minimum bias events becomes similar to the
             fairly constant ratio in jets at pT∼5 GeV/c. This suggests
             that the particles with pTâ‰35 GeV/c in minimum bias
             events are from "soft" jets, and that the pT slope of
             particles in jets is insensitive to light quark flavor (u,
             d, or s) and to the number of valence quarks. We also find
             that for pT≠24 GeV relatively more Λ0 baryons are
             produced in minimum bias events than in jets. © 2013
             American Physical Society.},
   Doi = {10.1103/PhysRevD.88.092005},
   Key = {fds310397}
}

@article{fds341955,
   Author = {Aaltonen, T and González, BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and Barbaro, PD and Cecco,
             SD and Lorenzo, GD and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'errico, M and Canto, AD and Ruzza, BD and Dittmann, JR and D'onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
             R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
             S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
             MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum, W and Keung,
             J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
             M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, C and Liu, Q and Liu, T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Maksimovic, P and Malik, S and Manca, G and Manousakis-Katsikakis,
             A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson,
             ME and Mazzanti, P and Mcfarland, KS and Mcintyre, P and Mcnulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin,
             F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa,
             K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson,
             GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel,
             M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, C and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wen, A and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund,
             AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson,
             JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka,
             J},
   Title = {Production of Λ0, Λ ̄0, Ξ ±, and
             Ω± hyperons in pp̄ collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {1},
   Year = {2012},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.012002},
   Abstract = {We report a set of measurements of inclusive invariant p T
             differential cross sections of Λ0, Λ ̄0, Ξ ±, and Ω ±
             hyperons reconstructed in the central region with
             pseudorapidity |η|&lt;1 and p T up to 10GeV/c. Events are
             collected with a minimum-bias trigger in pp̄ collisions at
             a center-of-mass energy of 1.96 TeV using the CDF II
             detector at the Tevatron Collider. As p T increases, the
             slopes of the differential cross sections of the three
             particles are similar, which could indicate a universality
             of the particle production in p T. The invariant
             differential cross sections are also presented for different
             charged-particle multiplicity intervals. © 2012 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.86.012002},
   Key = {fds341955}
}

@article{fds307990,
   Author = {Aaltonen, T and others},
   Title = {Production of ψ(2S) mesons in pp̅ collisions at 1.96
             TeV},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {3},
   Pages = {031103},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.031103},
   Abstract = {We have measured the differential cross section for the
             inclusive production of ψ(2S) mesons decaying to μ+μ-
             that were produced in prompt or B-decay processes from pp̅
             collisions at 1.96 TeV. These measurements have been made
             using a data set from an integrated luminosity of
             1.1  fb-1 collected by the CDF II detector at Fermilab.
             For events with transverse momentum pT(ψ(2S))&gt;2  GeV/c
             and rapidity |y(ψ(2S))|&lt;0.6 we measure the integrated
             inclusive cross section σ(pp̅ →ψ(2S)X)·Br(ψ(2S)→μ+μ-)
             to be 3.29 &plusmn; 0.04(stat) &plusmn; 0.32(syst)  nb.},
   Doi = {10.1103/PhysRevD.80.031103},
   Key = {fds307990}
}

@article{fds372393,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
             Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
             JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF},
   Title = {Production of ϒ(nS) mesons in Pb + Pb and pp collisions at
             5.02 TeV},
   Journal = {Physical Review C},
   Volume = {107},
   Number = {5},
   Year = {2023},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevC.107.054912},
   Abstract = {A measurement of the production of vector bottomonium
             states, ϒ(1S), ϒ(2S), and ϒ(3S), in Pb + Pb and pp
             collisions at a center-of-mass energy per nucleon pair of
             5.02 TeV is presented. The data correspond to integrated
             luminosities of 1.38 nb-1 of Pb + Pb data collected in 2018,
             0.44 nb-1 of Pb + Pb data collected in 2015, and 0.26 fb-1
             of pp data collected in 2017 by the ATLAS detector at the
             Large Hadron Collider. The measurements are performed in the
             dimuon decay channel for transverse momentum pμμT < 30
             GeV, absolute rapidity |yμμ| < 1.5, and Pb + Pb event
             centrality 0-80%. The production rates of the three
             bottomonium states in Pb + Pb collisions are compared with
             those in pp collisions to extract the nuclear modification
             factors as functions of event centrality, pμμT, and
             |yμμ|. In addition, the suppression of the excited states
             relative to the ground state is studied. The results are
             compared with theoretical model calculations.},
   Doi = {10.1103/PhysRevC.107.054912},
   Key = {fds372393}
}

@article{fds347480,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Pereira, RA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
             J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez,
             O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou,
             EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Gupta, DB and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
             G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous,
             S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot,
             C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
             O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RMB and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
             KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt,
             A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
             DL and Bristow, TM and Britton, D and Britzger, D and Brock, I and Brock,
             R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni,
             A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
             MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard,
             CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
             BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
             S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F},
   Title = {Prompt and non-prompt J / ψ and ψ ( 2 S ) suppression at
             high transverse momentum in 5.02 TeV Pb+Pb collisions with
             the ATLAS experiment.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {9},
   Pages = {762},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-6219-9},
   Abstract = {A measurement of J / ψ and ψ ( 2 S ) production is
             presented. It is based on a data sample from Pb+Pb
             collisions at s NN = 5.02 TeV and <i>pp</i> collisions at s
             = 5.02 TeV recorded by the ATLAS detector at the LHC in
             2015, corresponding to an integrated luminosity of 0.42 nb -
             1 and 25 pb - 1 in Pb+Pb and <i>pp</i>, respectively. The
             measurements of per-event yields, nuclear modification
             factors, and non-prompt fractions are performed in the
             dimuon decay channel for 9 < p T μ μ < 40 GeV in dimuon
             transverse momentum, and - 2 < y μ μ < 2 in rapidity.
             Strong suppression is found in Pb+Pb collisions for both
             prompt and non-prompt J / ψ , increasing with event
             centrality. The suppression of prompt ψ ( 2 S ) is observed
             to be stronger than that of J / ψ , while the suppression
             of non-prompt ψ ( 2 S ) is equal to that of the non-prompt
             J / ψ within uncertainties, consistent with the expectation
             that both arise from <i>b</i>-quarks propagating through the
             medium. Despite prompt and non-prompt J / ψ arising from
             different mechanisms, the dependence of their nuclear
             modification factors on centrality is found to be quite
             similar.},
   Doi = {10.1140/epjc/s10052-018-6219-9},
   Key = {fds347480}
}

@article{fds347479,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
             M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
             E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
             M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
             KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
             U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
             PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch,
             TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
             BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
             S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară,
             IA},
   Title = {Prompt and non-prompt J / ψ elliptic flow in Pb+Pb
             collisions at s NN = 5.02 Tev with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {9},
   Pages = {784},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-6243-9},
   Abstract = {The elliptic flow of prompt and non-prompt J / ψ was
             measured in the dimuon decay channel in Pb+Pb collisions at
             s NN = 5.02   TeV with an integrated luminosity of 0.42 nb
             - 1 with the ATLAS detector at the LHC. The prompt and
             non-prompt signals are separated using a two-dimensional
             simultaneous fit of the invariant mass and pseudo-proper
             decay time of the dimuon system from the J / ψ decay. The
             measurement is performed in the kinematic range of dimuon
             transverse momentum and rapidity 9 < p T < 30   GeV , | y |
             < 2 , and 0-60% collision centrality. The elliptic flow
             coefficient, v 2 , is evaluated relative to the event plane
             and the results are presented as a function of transverse
             momentum, rapidity and centrality. It is found that prompt
             and non-prompt J / ψ mesons have non-zero elliptic flow.
             Prompt J / ψ v 2 decreases as a function of p T , while for
             non-prompt J / ψ it is, with limited statistical
             significance, consistent with a flat behaviour over the
             studied kinematic region. There is no observed dependence on
             rapidity or centrality.},
   Doi = {10.1140/epjc/s10052-018-6243-9},
   Key = {fds347479}
}

@article{fds356621,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli,
             E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
             Pereira, R and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos,
             S},
   Title = {Properties of g →b b at small opening angles in pp
             collisions with the ATLAS detector at √s=13
             TeV},
   Journal = {Physical Review D},
   Volume = {99},
   Number = {5},
   Year = {2019},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.99.052004},
   Abstract = {The fragmentation of high-energy gluons at small opening
             angles is largely unconstrained by present measurements.
             Gluon splitting to b-quark pairs is a unique probe into the
             properties of gluon fragmentation because identified
             b-tagged jets provide a proxy for the quark daughters of the
             initial gluon. In this study, key differential distributions
             related to the g→bb process are measured using 33 fb-1 of
             s=13 TeV pp collision data recorded by the ATLAS experiment
             at the LHC in 2016. Jets constructed from charged-particle
             tracks, clustered with the anti-kt jet algorithm with radius
             parameter R=0.2, are used to probe angular scales below the
             R=0.4 jet radius. The observables are unfolded to particle
             level in order to facilitate direct comparisons with
             predictions from present and future simulations. Multiple
             significant differences are observed between the data and
             parton shower Monte Carlo predictions, providing input to
             improve these predictions of the main source of background
             events in analyses involving boosted Higgs bosons decaying
             into b-quarks.},
   Doi = {10.1103/PhysRevD.99.052004},
   Key = {fds356621}
}

@article{fds356573,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
             V},
   Title = {Properties of jet fragmentation using charged particles
             measured with the ATLAS detector in pp collisions at s =13
             TeV},
   Journal = {Physical Review D},
   Volume = {100},
   Number = {5},
   Year = {2019},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.100.052011},
   Abstract = {This paper presents a measurement of quantities related to
             the formation of jets from high-energy quarks and gluons
             (fragmentation). Jets with transverse momentum 100 GeV
             <pT<2.5 TeV and pseudorapidity |η|<2.1 from an integrated
             luminosity of 33 fb-1 of s=13 TeV proton-proton collisions
             are reconstructed with the ATLAS detector at the Large
             Hadron Collider. Charged-particle tracks with pT>500 MeV and
             |η|<2.5 are used to probe the detailed structure of the
             jet. The fragmentation properties of the more forward and
             the more central of the two leading jets from each event are
             studied. The data are unfolded to correct for detector
             resolution and acceptance effects. Comparisons with parton
             shower Monte Carlo generators indicate that existing models
             provide a reasonable description of the data across a wide
             range of phase space, but there are also significant
             differences. Furthermore, the data are interpreted in the
             context of quark- and gluon-initiated jets by exploiting the
             rapidity dependence of the jet flavor fraction. A first
             measurement of the charged-particle multiplicity using
             model-independent jet labels (topic modeling) provides a
             promising alternative to traditional quark and gluon
             extractions using input from simulation. The simulations
             provide a reasonable description of the quark-like data
             across the jet pT range presented in -this measurement, but
             the gluon-like data have systematically fewer charged
             particles than the simulation.},
   Doi = {10.1103/PhysRevD.100.052011},
   Key = {fds356573}
}

@article{fds307856,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Properties of jets measured from tracks in proton-proton
             collisions at center-of-mass energy √s=7TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {84},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2011},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.054001},
   Doi = {10.1103/PhysRevD.84.054001},
   Key = {fds307856}
}

@booklet{Adams96,
   Author = {Adams, MR and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dietrich, FS and Dougherty, W and Dreyer, T and Eckardt, V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen, KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Jackson, HE and Jaffe, DE and Jancso, G and Jansen, DM and Jin, Z and Kaufman, S and Kennedy, RD and Kinney, ER and Kobrak, HG and Kotwal, AV and Kunori, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin, JG and Nickerson, RB and Novak, J and O'Day, S and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou, V and Pawlik, B and Pipkin, FM and Potterveld, DH and Ramberg, EJ},
   Title = {Proton and deuteron structure functions in muon scattering
             at 470 GeV.},
   Journal = {Physical review. D, Particles and fields},
   Volume = {54},
   Number = {5},
   Pages = {3006-3056},
   Year = {1996},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevd.54.3006},
   Doi = {10.1103/physrevd.54.3006},
   Key = {Adams96}
}

@article{fds307966,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov,
             A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
   Title = {Publisher's Note: Search for hadronic decays of W and Z
             bosons in photon events in pp̄ collisions at
             s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {80},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.079901},
   Doi = {10.1103/PhysRevD.80.079901},
   Key = {fds307966}
}

@article{fds347512,
   Author = {Singhal, S and Bhattachar, SA and Paliwal, V and Malhotra, VK and Addya,
             K and Kotwal, A},
   Title = {Pulmonary Embolism in Young Natives of High
             Altitude.},
   Journal = {Heart views : the official journal of the Gulf Heart
             Association},
   Volume = {17},
   Number = {2},
   Pages = {62-65},
   Year = {2016},
   Month = {April},
   url = {http://dx.doi.org/10.4103/1995-705x.185115},
   Abstract = {Thrombotic events are relatively common in high altitude
             areas and known to occur in young soldiers working at high
             altitude without usual risk factors associated with
             thrombosis at sea-level. However, till now, cases with
             thrombotic events were reported only in lowlanders staying
             at high altitude. These two cases of pulmonary embolism
             demonstrate that thrombotic events can occur in highlanders
             after a prolonged stay at the extreme altitude.},
   Doi = {10.4103/1995-705x.185115},
   Key = {fds347512}
}

@article{fds308179,
   Author = {Abbott, B and Abdesselam, A and Abolins, M and Abramov, V and Acharya,
             BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar,
             V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler,
             M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MA and Cutts, D and Davis, GA and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
             T and Feher, S and Fein, D and Ferbel, T and Filthaut, F and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin,
             R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grünendahl, S and Gupta,
             A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hou, S and Huang, Y and Illingworth, R and Ito, AS and Jaffré, M and Jerger, SA and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Karmanov, D and Karmgard, D and Kim, SK and Klima, B and Klopfenstein, C and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov,
             AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski,
             S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kuznetsov, VE and Landsberg, G and Leflat, A and Leggett, C and Lehner,
             F and Li, J and Li, QZ and Lima, JG and Lincoln, D and Linn, SL and Linnemann,
             J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AK and Madaras, RJ and Manankov, V and Mao, HS and Marshall, T and Martin, MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy, R and McDonald, J and McMahon, T and Melanson, HL and Meng,
             XC and Merkin, M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea,
             D and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery, HE and Moore,
             RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Norman, D and Nunnemann, T and Oesch, L and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou, K and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Pétroff, P and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu,
             S and Qian, J and Quintas, PZ and Raja, R and Rajagopalan, S and Ramberg,
             E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell, RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery, P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon,
             J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Strovink, M and Stutte, L and Sznajder, A and Taylor, W and Tentindo-Repond, S and Thompson, J and Toback, D and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and van Gemmeren, P and Vaniev,
             V and Van Kooten and R and Varelas, N and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Wirjawan, JV and Womersley, J and Wood, DR and Yamada, R and Yamin, P and Yasuda, T and Yip,
             K and Youssef, S and Yu, J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev,
             EG and Zylberstejn, A},
   Title = {Quasi-model-independent search for new high p(T) physics at
             D0.},
   Journal = {Physical review letters},
   Volume = {86},
   Number = {17},
   Pages = {3712-3717},
   Year = {2001},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.86.3712},
   Abstract = {We apply a quasi-model-independent strategy ("Sleuth") to
             search for new high p(T) physics in approximately 100 pb(-1)
             of pp collisions at square root of (s) = 1.8 TeV collected
             by the D0 experiment during 1992-1996 at the Fermilab
             Tevatron. We systematically analyze many exclusive final
             states and demonstrate sensitivity to a variety of models
             predicting new phenomena at the electroweak scale. No
             evidence of new high p(T) physics is observed.},
   Doi = {10.1103/physrevlett.86.3712},
   Key = {fds308179}
}

@article{fds308188,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev,
             VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett,
             JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings,
             MAC and Cutts, D and Davis, GA and Davis, K and De, K and Jong, SJ and Del
             Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A},
   Title = {Quasi-model-independent search for new physics at large
             transverse momentum},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {64},
   Number = {1},
   Pages = {120041-1200424},
   Publisher = {American Physical Society (APS)},
   Year = {2001},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.64.012004},
   Abstract = {We apply a quasi-model-independent strategy (“SLEUTH”)
             to search for new high [Formula Presented] physics in ≈100
             [Formula Presented] of [Formula Presented] collisions at
             [Formula Presented] collected by the DØ experiment during
             1992–1996 at the Fermilab Tevatron. Over 32 [Formula
             Presented] [Formula Presented] [Formula Presented] and
             [Formula Presented] exclusive final states are
             systematically analyzed for hints of physics beyond the
             standard model. Simultaneous sensitivity to a variety of
             models predicting new phenomena at the electroweak scale is
             demonstrated by testing the method on a particular signature
             in each set of final states. No evidence of new high
             [Formula Presented] physics is observed in the course of
             this search, and we find that 89% of an ensemble of
             hypothetical similar experimental runs would have produced a
             final state with a candidate signal more interesting than
             the most interesting observed in these data. © 2001 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.64.012004},
   Key = {fds308188}
}

@article{fds307730,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Rapidity gap cross sections measured with the ATLAS detector
             in pp collisions at √s =7 TeV},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {3},
   Pages = {1-31},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-1926-0},
   Abstract = {Pseudorapidity gap distributions in proton-proton collisions
             at √s = 7 TeV are studied using a minimum bias data sample
             with an integrated luminosity of 7.1 μb<sup>−1</sup>.
             Cross sections are measured differentially in terms of
             Δη<sup>F</sup>, the larger of the pseudorapidity regions
             extending to the limits of the ATLAS sensitivity, at η =
             ±4.9, in which no final state particles are produced above
             a transverse momentum threshold p<sup>cut</sup><inf>T</inf>.
             The measurements span the region 0 < Δη<sup>F</sup> < 8
             for 200 MeV < p<sup>cut</sup><inf>T</inf> < 800 MeV. At
             small Δη<sup>F</sup>, the data test the reliability of
             hadronisation models in describing rapidity and transverse
             momentum fluctuations in final state particle production.
             The measurements at larger gap sizes are dominated by
             contributions from the single diffractive dissociation
             process (pp →Xp), enhanced by double dissociation (pp →
             XY) where the invariant mass of the lighter of the two
             dissociation systems satisfies M<inf>Y</inf> < 7 GeV. The
             resulting cross section is dσ/dΔη<sup>F</sup> ≈1 mb for
             Δη<sup>F</sup> > 3. The large rapidity gap data are used
             to constrain the value of the Pomeron intercept appropriate
             to triple Regge models of soft diffraction. The cross
             section integrated over all gap sizes is compared with other
             LHC inelastic cross section measurements.},
   Doi = {10.1140/epjc/s10052-012-1926-0},
   Key = {fds307730}
}

@article{fds346171,
   Author = {Patrikar, S and Basannar, DR and Bhatti, VK and Kotwal, A and Gupta, RM and Grewal, RS},
   Title = {Rate of decline in CD4 count in HIV patients not on
             antiretroviral therapy.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {70},
   Number = {2},
   Pages = {134-138},
   Year = {2014},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.mjafi.2013.08.005},
   Abstract = {<h4>Background</h4>The progressive decline in the CD4 count
             in HIV patients leads to a more general decline in immune
             functioning. The study has been carried out to determine the
             decline in CD4 count in HIV patients.<h4>Methods</h4>The
             study was conducted in a medical college hospital at
             Maharashtra. The information on baseline CD4 count was
             gathered from positive patient records registered in the
             central disease registry. The baseline CD4 count was the
             first count of CD4 obtained when the patient is diagnosed as
             HIV positive and further two subsequent readings. The time
             from baseline (t1) till the last CD4 count (t2) was divided
             into the different quartiles and the median decline in CD4
             count in each quartile was determined. As the time between
             the two CD4 count measurements was not uniform the rate of
             change in CD4 was measured with respect to time as [X
             (t2) - X (t1)/(t2 - t1)]. Correlation was assessed using
             correlation coefficient.<h4>Results</h4>As the CD4 counts
             were following skewed distribution, the normality was
             achieved by cuberoot transformation. The overall rate of
             decline in CD4 count was estimated to be 35 cells/μL per
             year with 95% confidence interval (CI) as (17.01, 85.04).
             The correlation coefficient between decline in CD4 and the
             initial CD4 count in the four time quartiles was
             (r = -0.51; p = 0.001, r = -0.79; p = 0.000,
             r = -0.48; p = 0.015 and r = -0.80; p = 0.000)
             respectively. The median decline in the CD4 count in 0-6
             months was 3 cells/μL, in (6-11) months was approximately
             26 cells/μL, in (11-21.5) months was 30 cells/μL and in
             more than 21.5 months the median decline was 52
             cells/μL.<h4>Conclusions</h4>There was a progressive
             decline in the CD4 count following HIV infection. An
             understanding of the influence of decline in CD4 count in
             HIV patients not on ART is important for clinical management
             of HIV disease.},
   Doi = {10.1016/j.mjafi.2013.08.005},
   Key = {fds346171}
}

@article{fds331391,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon,
             TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
             VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
             F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and De Jong and SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros,
             Y},
   Title = {Ratio of isolated photon cross sections in pp¯
             Collisions at √s = 630 and 1800 GeV},
   Journal = {Physical Review Letters},
   Volume = {87},
   Number = {25},
   Pages = {251805-1-251805-7},
   Publisher = {American Physical Society (APS)},
   Year = {2001},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevLett.87.251805},
   Abstract = {The inclusive cross section for production of isolated
             photons has been measured in pp¯ collisions at √s = 630
             GeV with the D0 detector at the Fermilab Tevatron Collider.
             The photons span a transverse energy (ET) range from 7-49
             GeV and have pseudorapidity |η| < 2.5. This measurement is
             combined with the previous D0 result at √s = 1800 GeV to
             form a ratio of the cross sections. Comparison of
             next-to-leading-order QCD with the measured cross section at
             630 GeV and the ratio of cross sections show satisfactory
             agreement in most of the ET range. © 2001 American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.87.251805},
   Key = {fds331391}
}

@article{fds308191,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
             JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
             R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
             D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MA and Cutts, D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gibbard, B and Gilmartin, R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grudberg, P and Grünendahl, S and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hou, S and Huang, Y and Ito, AS and Jerger, SA and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Karmanov, D and Karmgard, D and Kehoe, R and Kim, SK and Klima, B and Klopfenstein, C and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kuznetsov, VE and Landsberg, G and Leflat, A and Lehner,
             F and Li, J and Li, QZ and Lima, JG and Lincoln, D and Linn, SL and Linnemann,
             J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Maciel,
             AK and Madaras, RJ and Manankov, V and Mao, HS and Marshall, T and Martin,
             MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy,
             R and McDonald, J and McMahon, T and Melanson, HL and Meng, XC and Merkin,
             M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea, D and Mincer,
             A and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery, HE and Moore,
             RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Norman, D and Oesch, L and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan,
             LJ and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno,
             M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Qian, J and Quintas, PZ and Raja, R and Rajagopalan,
             S and Ramberg, E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Schwartzman, A and Sculli, J and Sen, N and Shabalina,
             E and Shankar, HC and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell,
             RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery,
             P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stevenson, ML and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Streets, K and Strovink,
             M and Stutte, L and Sznajder, A and Taylor, W and Tentindo-Repond, S and Thompson, J and Toback, D and Tripathi, SM and Trippe, TG and Turcot,
             AS and Tuts, PM and van Gemmeren, P and Vaniev, V and Van Kooten and R and Varelas, N and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White,
             A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Wirjawan, JV and Womersley, J and Wood,
             DR and Yamada, R and Yamin, P and Yasuda, T and Yip, K and Youssef, S and Yu,
             J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zhu, ZH and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev,
             EG and Zylberstejn, A and D0 Collaboration},
   Title = {Ratio of jet cross sections at square root of s = 630 GeV
             and 1800 GeV.},
   Journal = {Physical review letters},
   Volume = {86},
   Number = {12},
   Pages = {2523-2528},
   Year = {2001},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.86.2523},
   Abstract = {The D0 Collaboration has measured the inclusive jet cross
             section in barpp collisions at square root of s = 630 GeV.
             The results for pseudorapidities (eta)<0.5 are combined with
             our previous results at square root of s = 1800 GeV to form
             a ratio of cross sections with smaller uncertainties than
             either individual measurement. Next-to-leading-order QCD
             predictions show excellent agreement with the measurement at
             630 GeV; agreement is also satisfactory for the ratio.
             Specifically, despite a 10% to 15% difference in the
             absolute magnitude, the dependence of the ratio on jet
             transverse momentum is very similar for data and
             theory.},
   Doi = {10.1103/physrevlett.86.2523},
   Key = {fds308191}
}

@article{fds308181,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
             JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
             R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
             D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MA and Cutts, D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gibbard, B and Gilmartin, R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grudberg, P and Grünendahl, S and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hou, S and Huang, Y and Ito, AS and Jerger, SA and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Karmanov, D and Karmgard, D and Kehoe, R and Kim, SK and Klima, B and Klopfenstein, C and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kuznetsov, VE and Landsberg, G and Leflat, A and Lehner,
             F and Li, J and Li, QZ and Lima, JG and Lincoln, D and Linn, SL and Linnemann,
             J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Maciel,
             AK and Madaras, RJ and Manankov, V and Mao, HS and Marshall, T and Martin,
             MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy,
             R and McDonald, J and McMahon, T and Melanson, HL and Meng, XC and Merkin,
             M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea, D and Mincer,
             A and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery, HE and Moore,
             RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Norman, D and Oesch, L and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan,
             LJ and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno,
             M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Qian, J and Quintas, PZ and Raja, R and Rajagopalan,
             S and Ramberg, E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Schwartzman, A and Sculli, J and Sen, N and Shabalina,
             E and Shankar, HC and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell,
             RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery,
             P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stevenson, ML and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Streets, K and Strovink,
             M and Stutte, L and Sznajder, A and Taylor, W and Tentindo-Repond, S and Thompson, J and Toback, D and Tripathi, SM and Trippe, TG and Turcot,
             AS and Tuts, PM and van Gemmeren, P and Vaniev, V and Van Kooten and R and Varelas, N and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White,
             A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Wirjawan, JV and Womersley, J and Wood,
             DR and Yamada, R and Yamin, P and Yasuda, T and Yip, K and Youssef, S and Yu,
             J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zhu, ZH and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev,
             EG and Zylberstejn, A},
   Title = {Ratios of multijet Cross Sections in p p collisions at
             radical(s) = 1.8 TeV.},
   Journal = {Physical review letters},
   Volume = {86},
   Number = {10},
   Pages = {1955-1960},
   Year = {2001},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.86.1955},
   Abstract = {We report on a study of the ratio of inclusive three-jet to
             inclusive two-jet production cross sections as a function of
             total transverse energy in p&pmacr; collisions at a
             center-of-mass energy sqrt[s] = 1.8 TeV, using data
             collected with the D0 detector during the 1992-1993 run of
             the Fermilab Tevatron Collider. The measurements are used to
             deduce preferred renormalization scales in perturbative
             O(alpha(3)(s)) QCD calculations in modeling soft-jet
             emission.},
   Doi = {10.1103/physrevlett.86.1955},
   Key = {fds308181}
}

@article{fds354162,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
             C},
   Title = {Reconstruction and identification of boosted di-τ systems
             in a search for Higgs boson pairs using 13 TeV proton-proton
             collision data in ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {11},
   Year = {2020},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2020)163},
   Abstract = {In this paper, a new technique for reconstructing and
             identifying hadronically decaying τ+τ− pairs with a
             large Lorentz boost, referred to as the di-τ tagger, is
             developed and used for the first time in the ATLAS
             experiment at the Large Hadron Collider. A benchmark di-τ
             tagging selection is employed in the search for resonant
             Higgs boson pair production, where one Higgs boson decays
             into a boosted bb¯ pair and the other into a boosted
             τ+τ− pair, with two hadronically decaying τ-leptons in
             the final state. Using 139 fb−1 of proton-proton collision
             data recorded at a centre-of-mass energy of 13 TeV, the
             efficiency of the di-τ tagger is determined and the
             background with quark- or gluon-initiated jets misidentified
             as di-τ objects is estimated. The search for a heavy,
             narrow, scalar resonance produced via gluon-gluon fusion and
             decaying into two Higgs bosons is carried out in the mass
             range 1–3 TeV using the same dataset. No deviations from
             the Standard Model predictions are observed, and 95%
             confidence-level exclusion limits are set on this model.
             [Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP11(2020)163},
   Key = {fds354162}
}

@article{fds316852,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus,
             M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
             S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
             K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
             J},
   Title = {Reconstruction of hadronic decay products of tau leptons
             with the ATLAS experiment.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {295},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4110-0},
   Abstract = {This paper presents a new method of reconstructing the
             individual charged and neutral hadrons in tau decays with
             the ATLAS detector. The reconstructed hadrons are used to
             classify the decay mode and to calculate the visible
             four-momentum of reconstructed tau candidates, significantly
             improving the resolution with respect to the calibration in
             the existing tau reconstruction. The performance of the
             reconstruction algorithm is optimised and evaluated using
             simulation and validated using samples of [Formula: see
             text] and [Formula: see text]+jets events selected from
             proton-proton collisions at a centre-of-mass energy
             [Formula: see text], corresponding to an integrated
             luminosity of 5 [Formula: see text].},
   Doi = {10.1140/epjc/s10052-016-4110-0},
   Key = {fds316852}
}

@article{fds347500,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
             Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
             A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL},
   Title = {Reconstruction of primary vertices at the ATLAS experiment
             in Run 1 proton-proton collisions at the
             LHC.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {5},
   Pages = {332},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4887-5},
   Abstract = {This paper presents the method and performance of primary
             vertex reconstruction in proton-proton collision data
             recorded by the ATLAS experiment during Run 1 of the LHC.
             The studies presented focus on data taken during 2012 at a
             centre-of-mass energy of [Formula: see text] TeV. The
             performance has been measured as a function of the number of
             interactions per bunch crossing over a wide range, from one
             to seventy. The measurement of the position and size of the
             luminous region and its use as a constraint to improve the
             primary vertex resolution are discussed. A longitudinal
             vertex position resolution of about [Formula: see text] is
             achieved for events with high multiplicity of reconstructed
             tracks. The transverse position resolution is better than
             [Formula: see text] and is dominated by the precision on the
             size of the luminous region. An analytical model is proposed
             to describe the primary vertex reconstruction efficiency as
             a function of the number of interactions per bunch crossing
             and of the longitudinal size of the luminous region.
             Agreement between the data and the predictions of this model
             is better than 3% up to seventy interactions per bunch
             crossing.},
   Doi = {10.1140/epjc/s10052-017-4887-5},
   Key = {fds347500}
}

@article{fds346213,
   Author = {Bains, R and Kotwal, A and Saeed, W},
   Title = {Recurrent carpal tunnel syndrome in a child due to
             fibrolipomatous hamartoma of the median nerve successfully
             treated by limited excision and decompression.},
   Journal = {Journal of plastic, reconstructive & aesthetic surgery :
             JPRAS},
   Volume = {59},
   Number = {12},
   Pages = {1394-1397},
   Year = {2006},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.bjps.2006.01.016},
   Abstract = {We present a case of recurrent carpal tunnel syndrome in a
             child caused by fibrolipomatous hamartoma of the median
             nerve which was successfully treated by limited excision of
             the fibrolipomatous tissue and decompression.},
   Doi = {10.1016/j.bjps.2006.01.016},
   Key = {fds346213}
}

@article{fds346175,
   Author = {Shega, JW and Andrew, M and Kotwal, A and Lau, DT and Herr, K and Ersek, M and Weiner, DK and Chin, MH and Dale, W},
   Title = {Relationship between persistent pain and 5-year mortality: a
             population-based prospective cohort study.},
   Journal = {Journal of the American Geriatrics Society},
   Volume = {61},
   Number = {12},
   Pages = {2135-2141},
   Year = {2013},
   Month = {December},
   url = {http://dx.doi.org/10.1111/jgs.12554},
   Abstract = {<h4>Objectives</h4>To assess the association between
             self-reported noncancer pain and 5-year mortality.<h4>Design</h4>Cohort.<h4>Setting</h4>Community-dwelling
             older adults.<h4>Participants</h4>Canadian Study of Health
             and Aging 1996 wave.<h4>Measurements</h4>Registrar of Vital
             Statistics-established 5-year mortality. Noncancer pain was
             assessed using the 5-point verbal descriptor scale,
             dichotomized into no or very mild versus moderate, severe,
             or very severe pain. Frailty was the accumulation of health
             deficits. Cognitive status (Modified Mini-Mental State
             Examination) and depressed mood (five-item mental health
             screening questionnaire) were also assessed. Multivariable
             logistic regression and Cox proportional hazards were used
             to analyze the relationship between pain and 5-year
             mortality.<h4>Results</h4>Of 5,703 participants, 4,694
             (82.3%) had complete data for analysis; 1,663 of these
             (35.4%) reported moderate, severe, or very severe pain, and
             1,343 (28.6%) had died at 5-year follow-up. Four hundred
             ninety-six of those who died (29.8%) reported moderate,
             severe, or very severe pain and 847 (27.9%) no or very mild
             pain. Multivariate logistic analysis found that individuals
             with moderate, severe, or very severe pain had lower odds of
             5-year mortality than those with no or very mild pain (odds
             ratio=0.78, 95% confidence interval (CI)=0.66-0.92; P<.001).
             The risk of death was lower in persons reporting moderate or
             greater pain than in those with no or very mild pain
             (HR=0.85, 95% CI=0.75-0.96; P=.01). An interaction between
             pain and sex explained this effect. Men with pain were not
             significantly more likely than men without pain to die
             (HR=1.00, 95% CI=0.84-1.19; P=.99), whereas women without
             pain (HR=0.54, 95% CI=0.47-0.63; P<0.01) and women with pain
             (HR=0.40; CI=0.33-0.47; P<.01) had less risk of death than
             men without and with pain, respectively.<h4>Conclusion</h4>Older
             women with pain were less likely to die within 5 years than
             older women without pain, men in pain, or men without
             pain.},
   Doi = {10.1111/jgs.12554},
   Key = {fds346175}
}

@article{fds346209,
   Author = {Varma, PP and Hooda, AK and Sinha, T and Chopra, GS and Karan, SC and Sethi, GS and Badwal, S and Kotwal, A},
   Title = {Renal Transplantation - An Experience of 500
             Patients.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {63},
   Number = {2},
   Pages = {107-111},
   Year = {2007},
   Month = {April},
   url = {http://dx.doi.org/10.1016/s0377-1237(07)80049-9},
   Abstract = {<h4>Background</h4>Renal transplantation is the treatment
             modality of choice for patients with end stage kidney
             failure. We present our experience of graft and patient
             survival of initial 500 renal transplants performed between
             May 1991 and July 2006, at Army Hospital (R&R).<h4>Material
             and methods</h4>All patients received triple drug
             immunosuppression with cyclosporine/tacrolimus,
             azathioprine/ mycophenolate mofetil and steroids. Patients
             in high risk group received induction therapy with IL-2
             receptor blockers/anti-thymocyte globulin.<h4>Results</h4>Majority
             of the recipients (79%) were males, whereas majority of the
             donors (59.4%) were females. In the donor profile, 385 (77%)
             transplants were live related, 108 (21.6 %) were spousal and
             7 (1.4%) were cadaveric transplants. Mean age of the donors
             and recipients was 42.11 ± 11.53 years (range 19-72 years)
             and 33 ± 9.39 years (range 5-60 years) respectively. Eighty
             two patients (16.4%) were lost to follow up and the present
             data on rejections, patients and graft survival pertains to
             418 patients. These patients have been followed up for a
             mean period of 2.63 years (SE, 0.122; median 1.8 years;
             range 0-13.36 years). Acute rejection episodes occurred in
             115 (27.3%) patients and 95% of these could be reversed with
             steroids/ATG. Sixty eight patients (16%) have died on
             follow-up. Our one-year, 5 year and 10 year estimated graft
             survival is 95.4% (SE, 0.01), 80.5% (SE, 0.03) and 53.1%
             (SE, 0.09) respectively and patient survival at one year is
             93.2% (SE, 0.01). The estimated graft and patient survival
             in our series is 9.83 (95% CI, 8.92-10.73) and 9.80
             (8.93-10.67) years respectively.<h4>Conclusion</h4>This
             centre's short-term graft survival of 95.4% is comparable to
             the best centres of the world.},
   Doi = {10.1016/s0377-1237(07)80049-9},
   Key = {fds346209}
}

@article{fds347515,
   Author = {Kotwal, A},
   Title = {Reply to: Regarding the Article: Does Iodine Excess Lead to
             Hypothyroidism? Evidence from A Case-Control Study in
             India.},
   Journal = {Archives of medical research},
   Volume = {47},
   Number = {2},
   Pages = {146-147},
   Year = {2016},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.arcmed.2016.05.003},
   Doi = {10.1016/j.arcmed.2016.05.003},
   Key = {fds347515}
}

@article{fds356574,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
             L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
             JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
             JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
             VA},
   Title = {Resolution of the ATLAS muon spectrometer monitored drift
             tubes in LHC Run 2},
   Journal = {Journal of Instrumentation},
   Volume = {14},
   Number = {9},
   Year = {2019},
   Month = {September},
   url = {http://dx.doi.org/10.1088/1748-0221/14/09/P09011},
   Abstract = {The momentum measurement capability of the ATLAS muon
             spectrometer relies fundamentally on the intrinsic
             single-hit spatial resolution of the monitored drift tube
             precision tracking chambers. Optimal resolution is achieved
             with a dedicated calibration program that addresses the
             specific operating conditions of the 354 000 high-pressure
             drift tubes in the spectrometer. The calibrations consist of
             a set of timing offsets and drift time to drift distance
             transfer relations, and result in chamber resolution
             functions. This paper describes novel algorithms to obtain
             precision calibrations from data collected by ATLAS in LHC
             Run 2 and from a gas monitoring chamber, deployed in a
             dedicated gas facility. The algorithm output consists of a
             pair of correction constants per chamber which are applied
             to baseline calibrations, and determined to be valid for the
             entire ATLAS Run 2. The final single-hit spatial resolution,
             averaged over 1172 monitored drift tube chambers, is 81.7 ±
             2.2 μm.},
   Doi = {10.1088/1748-0221/14/09/P09011},
   Key = {fds356574}
}

@article{fds346208,
   Author = {Anand, SS and Sood, V and Kumar, PG and Sinha, I and Kotwal,
             A},
   Title = {Retrospective Analysis of Thyroid Cancer
             Patients.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {64},
   Number = {1},
   Pages = {7-10},
   Year = {2008},
   Month = {January},
   url = {http://dx.doi.org/10.1016/s0377-1237(08)80136-0},
   Abstract = {<h4>Background</h4>Thyroid cancer is a spectrum of neoplasms
             and manifests in varied forms. The issues related to
             presentation, management and outcome of patients with
             thyroid malignancy are highlighted.<h4>Methods</h4>Retrospective
             analysis of 70 patients and survival analysis for event free
             survival was done.<h4>Result</h4>Papillary carcinomas
             constituted 88 percent followed by follicular cancers at
             nine percent of all cancers. Females were affected more than
             males in the ratio of 2.2: 1. Mean age of presentation for
             papillary cancer was 39 years and for follicular 50 years.
             Sixteen percent patients had regional and 10 percent distant
             metastases. Seventeen percent showed raised serum
             thyroglobulin and 29 percent had an abnormal whole body scan
             during the follow up. Relapse rate were similar in those
             receiving 30 mCi of radioiodine and in those receiving more
             than 30 mCi.<h4>Conclusion</h4>The study shows that tumour
             marker thyroglobulin has higher negative predictive value.
             Overall prognosis for differentiated thyroid cancers is
             good.},
   Doi = {10.1016/s0377-1237(08)80136-0},
   Key = {fds346208}
}

@article{fds310300,
   Author = {Bandurin, D and Bernardi, G and Gerber, C and Junk, T and Juste, A and Kotwal, A and Lewis, J and Mesropian, C and Schellman, H and Sekaric, J and Toback, D and Van Kooten and R and Vellidis, C and Zivkovic,
             L},
   Title = {Review of physics results from the Tevatron},
   Journal = {International Journal of Modern Physics A},
   Volume = {30},
   Number = {6},
   Pages = {1541001-1541001},
   Publisher = {World Scientific Pub Co Pte Lt},
   Year = {2015},
   Month = {February},
   ISSN = {0217-751X},
   url = {http://dx.doi.org/10.1142/S0217751X15410018},
   Abstract = {We present a comprehensive review of the physics results
             obtained by the CDF and D0 collaborations up to summer 2014,
             with emphasis on those achieved in the Run II of the
             Tevatron collider which delivered a total integrated
             luminosity of 10 fb-1 at $\sqrt{s} = 1.96~{\rm TeV}$. The
             results are presented in six main physics topics: QCD, Heavy
             Flavor, Electroweak, Top quark, Higgs boson and searches for
             New Particles and Interactions. The characteristics of the
             accelerator, detectors, and the techniques used to achieve
             these results are also briefly summarized.},
   Doi = {10.1142/S0217751X15410018},
   Key = {fds310300}
}

@article{fds310314,
   Author = {Kotwal, AV and Schellman, H and Sekaric, J},
   Title = {Review of physics results from the Tevatron: Electroweak
             physics},
   Journal = {International Journal of Modern Physics A},
   Volume = {30},
   Number = {6},
   Year = {2015},
   Month = {February},
   url = {http://dx.doi.org/10.1142/S0217751X15410043},
   Abstract = {We summarize an extensive Tevatron (1984-2011) electroweak
             physics program that involves a variety of W and Z boson
             precision measurements. The relevance of these studies using
             single and associated gauge boson production to our
             understanding of the electroweak sector, quantum
             chromodynamics and searches for new physics is emphasized.
             We discuss the importance of the W boson mass measurement,
             the W/Z boson distributions and asymmetries, and diboson
             studies. We highlight the recent Tevatron measurements and
             prospects for the final Tevatron measurements.},
   Doi = {10.1142/S0217751X15410043},
   Key = {fds310314}
}

@article{fds346187,
   Author = {Gupta, SK and Kotwal, J and Kotwal, A and Dhall, A and Garg,
             S},
   Title = {Role of homocysteine & MTHFR C677T gene polymorphism as risk
             factors for coronary artery disease in young
             Indians.},
   Journal = {The Indian journal of medical research},
   Volume = {135},
   Number = {4},
   Pages = {506-512},
   Year = {2012},
   Month = {April},
   Abstract = {<h4>Background & objectives</h4>Hyperhomocysteinaemia (HCA)
             either due to mutation of MTHFR gene or deficiency of
             vitamin B 12 and folic acid, has been reported as a risk
             factor for coronary artery disease (CAD). The present study
             was aimed to determine plasma homocysteine (Hcy) levels and
             to evaluate MTHFR C677T gene polymorphism as risk factors
             for CAD, and to study the role of Hcy in conjunction with a
             few other risk factors of CAD in young Indians. The effect
             of vitamin B12 and folic acid supplements on the raised
             plasma Hcy levels in patients of CAD was also
             assessed.<h4>Methods</h4>The present study included 199
             consecutive angiography confirmed CAD patients, <45 yr of
             age, without any other known pro- coagulant state and 200
             age- and sex-matched healthy controls. Fasting blood samples
             were collected in EDTA and plasma Hcy was estimated by ELISA
             test and the MTHFR C677T polymorphism detection was carried
             out by PCR-RFLP method.<h4>Results</h4>Significant
             difference (P<0.001) was found between mean fasting levels
             of plasma Hcy in cases (22.14 ± 10.62 μmol/l) and controls
             (17.38 ± 8.46 μmol/l) with an Odds ratio as 1.93 (95% CI,
             1.27-2.94). Levels of cholesterol, LDL, and triglycerides
             were significantly (P<0.001) higher in cases compared with
             controls.<h4>Interpretation & conclusions</h4>Our study
             showed significant correlation between hyperhomocysteinaemia
             and coronary artery disease. Multivariate analysis by
             logistic regression of the various risk factors of CAD,
             found high levels of Hcy, cholesterol, LDL and low levels of
             HDL and smoking as independent predictors of CAD when all
             other factors were controlled. Significant post-treatment
             decrease found in HCA was easily modifiable by vitamin
             intervention irrespective to their CT or TT genotype of
             C677T MTHFR gene. Further studies to look at the plasma
             levels of folate and cobalamines and their association with
             Hcy are required to be done.},
   Key = {fds346187}
}

@article{fds373611,
   Author = {Kotwal, AV and Matias, J and Mauri, A and Tong, T and Varnhorst,
             L},
   Title = {Round table on Standard Model Anomalies},
   Journal = {15th Conference on Quark Confinement and the Hadron
             Spectrum, Confinement 2022},
   Year = {2022},
   Month = {January},
   url = {http://dx.doi.org/10.1051/epjconf/202227401006},
   Abstract = {This contribution to “The XVth Quark confinement and the
             Hadron spectrum conference" covers a description, both
             theoretical and experimental, of the present status of a set
             of very different anomalies. The discussion ranges from the
             long standing b → sℓℓ anomalies, (g − 2) and the new
             MW anomaly.},
   Doi = {10.1051/epjconf/202227401006},
   Key = {fds373611}
}

@article{fds307896,
   Author = {Aaltonen, and T, and others},
   Title = {Search for $R$-Parity Violating Decays of Sneutrinos to
             $e\mu{}$, $\mu{}\tau{}$, and $e\tau{}$ Pairs in $pp[over
             \ifmmode\bar\else\textasciimacron\fi{}]$ Collisions at
             $\sqrt{s}=1.96\,\,TeV$},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {19},
   Pages = {191801},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.191801},
   Abstract = {We present a search for supersymmetric neutrino ν
             production using the Tevatron pp collision data collected
             with the CDF II detector and corresponding to an integrated
             luminosity of 1 fb-1. We focus on the scenarios predicted by
             the R-parity violating (RPV) supersymmetric models in which
             sneutrinos decay to two charged leptons of different flavor.
             With the data consistent with the standard model
             expectations, we set upper limits on σ(pp→ν)×BR(ν→eμ,μτ,eτ)
             and use these results to constrain the RPV couplings as a
             function of the sneutrino mass.},
   Doi = {10.1103/PhysRevLett.105.191801},
   Key = {fds307896}
}

@article{fds307903,
   Author = {Aaltonen, and T, and others},
   Title = {Search for $WW$ and $WZ$ resonances decaying to electron,
             missing $E_T$, and two jets in $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {24},
   Pages = {241801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.241801},
   Abstract = {http://arxiv.org/abs/1004.4946},
   Doi = {10.1103/PhysRevLett.104.241801},
   Key = {fds307903}
}

@article{fds308092,
   Author = {Abulencia, and A, and others},
   Title = {Search for $Z^\prime \to e^+ e^-$ using dielectron mass and
             angular distribution},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {21},
   Pages = {211801},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.211801},
   Abstract = {We report results from a search for Z' bosons in high-mass
             dielectron events produced in p anti-p collisions at
             s**(1/2) = 1.96 TeV. The data were recorded with the CDF II
             detector at the Fermilab Tevatron and correspond to an
             integrated luminosity of 0.45 fb-1. To identify the Z' -->
             e+ e- signal, both the dielectron invariant mass
             distribution and the angular distribution of the electron
             pair are used. No evidence for a signal is found, and 95\%
             confidence level lower limits are set on the Z' mass for
             several models.},
   Doi = {10.1103/physrevlett.96.211801},
   Key = {fds308092}
}

@article{fds310277,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM},
   Title = {Search for a Charged Higgs Boson Produced in the
             Vector-Boson Fusion Mode with Decay H(±)→W(±)Z using pp
             Collisions at √s=8  TeV with the ATLAS
             Experiment.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {23},
   Pages = {231801},
   Year = {2015},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.114.231801},
   Abstract = {A search for a charged Higgs boson, H(±), decaying to a
             W(±) boson and a Z boson is presented. The search is based
             on 20.3  fb(-1) of proton-proton collision data at a
             center-of-mass energy of 8 TeV recorded with the ATLAS
             detector at the LHC. The H(±) boson is assumed to be
             produced via vector-boson fusion and the decays W(±)→qq'
             and Z→e(+)e(-)/μ(+)μ(-) are considered. The search is
             performed in a range of charged Higgs boson masses from 200
             to 1000 GeV. No evidence for the production of an H(±)
             boson is observed. Upper limits of 31-1020 fb at 95% C.L.
             are placed on the cross section for vector-boson fusion
             production of an H(±) boson times its branching fraction to
             W(±)Z. The limits are compared with predictions from the
             Georgi-Machacek Higgs triplet model.},
   Doi = {10.1103/physrevlett.114.231801},
   Key = {fds310277}
}

@article{fds310285,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for a CP-odd Higgs boson decaying to Zh in pp
             collisions at √s=8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {744},
   Pages = {163-183},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.03.054},
   Abstract = {A search for a heavy, CP-odd Higgs boson, A, decaying into a
             Z boson and a 125 GeV Higgs boson, h, with the ATLAS
             detector at the LHC is presented. The search uses
             proton–proton collision data at a centre-of-mass energy of
             8 TeV corresponding to an integrated luminosity of 20.3
             fb−1. Decays of CP-even h bosons to ττ or bb pairs with
             the Z boson decaying to electron or muon pairs are
             considered, as well as h→bb decays with the Z boson
             decaying to neutrinos. No evidence for the production of an
             A boson in these channels is found and the 95% confidence
             level upper limits derived for σ(gg→A)×BR(A→Zh)×BR(h→ff¯)
             are 0.098–0.013 pb for f=τ and 0.57–0.014 pb for f=b in
             a range of mA=220–1000 GeV. The results are combined and
             interpreted in the context of two-Higgs-doublet
             models.},
   Doi = {10.1016/j.physletb.2015.03.054},
   Key = {fds310285}
}

@article{fds307704,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Anzá, F and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Fuks, B and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Search for a dark matter candidate produced in association
             with a single top quark in pp collisions at
             √[s]=1.96  TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {20},
   Pages = {201802},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.201802},
   Abstract = {We report a new search for dark matter in a data sample of
             an integrated luminosity of 7.7  fb-1 of Tevatron
             pp[over ¯] collisions at √[s]=1.96  TeV, collected by
             the CDF II detector. We search for production of a
             dark-matter candidate, D, in association with a single top
             quark. We consider the hadronic decay mode of the top quark
             exclusively, yielding a final state of three jets with
             missing transverse energy. The data are consistent with the
             standard model; we thus set 95% confidence level upper
             limits on the cross section of the process pp[over ¯]→t+D
             as a function of the mass of the dark-matter candidate. The
             limits are approximately 0.5 pb for a dark-matter particle
             with mass in the range of 0-150  GeV/c2.},
   Doi = {10.1103/physrevlett.108.201802},
   Key = {fds307704}
}

@article{fds307561,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Search for a dijet resonance in events with jets and missing
             transverse energy in pp̄ collisions at √s=1.96
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.092004},
   Abstract = {We report on a search for a dijet resonance in events with
             only two or three jets and a large imbalance in the total
             event transverse momentum. This search is sensitive to the
             possible production of a new particle in association with a
             W or Z boson, where the boson decays leptonically with one
             or more neutrinos in the final state. We use the full data
             set collected by the CDF II detector at the Tevatron
             collider at a proton-antiproton center-of-mass energy of
             1.96 TeV. These data correspond to an integrated luminosity
             of 9.1 fb -1. We study the invariant mass distribution of
             the two jets with highest transverse energy. We find good
             agreement between data and standard model background
             expectations and measure the combined cross section for WW,
             WZ, and ZZ production to be 13.8-2.7+3.0 pb. No significant
             anomalies are observed in the mass spectrum, and 95%
             credibility level upper limits are set on the production
             rates of a potential new particle in association with a W or
             Z boson. © 2013 American Physical Society.},
   Doi = {10.1103/PhysRevD.88.092004},
   Key = {fds307561}
}

@article{fds307946,
   Author = {Aaltonen, T and others},
   Title = {Search for a Fermiophobic Higgs Boson Decaying into
             Diphotons in pp̅ Collisions at sqrt[s]=1.96
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {6},
   Pages = {061803},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.061803},
   Abstract = {A search for a narrow diphoton mass resonance is presented
             based on data from 3.0  fb-1 of integrated luminosity
             from pp̅ collisions at sqrt[s]=1.96  TeV collected by
             the CDF experiment. No evidence of a resonance in the
             diphoton mass spectrum is observed, and upper limits are set
             on the cross section times branching fraction of the
             resonant state as a function of Higgs boson mass. The
             resulting limits exclude Higgs bosons with masses below
             106  GeV/c2 at a 95% Bayesian credibility level for one
             fermiophobic benchmark model.},
   Doi = {10.1103/physrevlett.103.061803},
   Key = {fds307946}
}

@article{fds307792,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
             A},
   Title = {Search for a fermiophobic Higgs boson in the diphoton decay
             channel with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {9},
   Pages = {1-18},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2157-0},
   Abstract = {A search for a fermiophobic Higgs boson using diphoton
             events produced in proton-proton collisions at a
             centre-of-mass energy of √s = 7 TeV is performed using
             data corresponding to an integrated luminosity of 4.9
             fb−1collected by the ATLAS experiment at the Large Hadron
             Collider. A specific benchmark model is considered where all
             the fermion couplings to the Higgs boson are set to zero and
             the bosonic couplings are kept at the Standard Model values
             (fermiophobic Higgs model). The largest excess with respect
             to the background-only hypothesis is found at 125.5 GeV,
             with a local significance of 2.9 standard deviations, which
             reduces to 1.6 standard deviations when taking into account
             the look-elsewhere effect. The data exclude the fermiophobic
             Higgs model in the ranges 110.0–118.0 GeV and
             119.5–121.0 GeV at 95 % confidence level.},
   Doi = {10.1140/epjc/s10052-012-2157-0},
   Key = {fds307792}
}

@booklet{Abachi97c,
   Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Boehnlein, AA and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg,
             M and Di Loreto and G and Draper, P and Drinkard, J and Alitti, J and Dudko,
             LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga, MK and Featherly,
             J and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y},
   Title = {Search for a Fourth Generation Charge -1/3 Quark via Flavor
             Changing Neutral Current Decay},
   Journal = {Physical Review Letters},
   Volume = {78},
   Number = {20},
   Pages = {3818-3823},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.78.3818},
   Abstract = {We report on a search for pair production of a fourth
             generation charge -1/3 quark (b’) in pp collisions at s =
             1.8 TeV by the DØ experiment at the Fermilab Tevatron using
             an integrated luminosity of 93 pb-1. Both b’ quarks are
             assumed to decay via flavor changing neutral currents
             (FCNC). The search uses the signatures γ + 3 jets + μ-tag
             and 2γ + 2 jets. We see no significant excess of events
             over the expected background. We place an upper limit on the
             production cross section times branching fraction that is
             well below theoretical expectations for a b’ decaying
             exclusively via FCNC for b’ masses up to mz + mb. © 1996
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.78.3818},
   Key = {Abachi97c}
}

@article{fds356572,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
             V},
   Title = {Search for a heavy charged boson in events with a charged
             lepton and missing transverse momentum from pp collisions at
             s =13 TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {100},
   Number = {5},
   Year = {2019},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.100.052013},
   Abstract = {A search for a heavy charged-boson resonance decaying into a
             charged lepton (electron or muon) and a neutrino is
             reported. A data sample of 139 fb-1 of proton-proton
             collisions at s=13 TeV collected with the ATLAS detector at
             the LHC during 2015-2018 is used in the search. The observed
             transverse mass distribution computed from the lepton and
             missing transverse momenta is consistent with the
             distribution expected from the Standard Model, and upper
             limits on the cross section for pp→W′→ℓν are
             extracted (ℓ=e or μ). These vary between 1.3 pb and 0.05
             fb depending on the resonance mass in the range between 0.15
             and 7.0 TeV at 95% confidence level for the electron and
             muon channels combined. Gauge bosons with a mass below 6.0
             and 5.1 TeV are excluded in the electron and muon channels,
             respectively, in a model with a resonance that has couplings
             to fermions identical to those of the Standard Model W
             boson. Cross-section limits are also provided for resonances
             with several fixed Γ/m values in the range between 1% and
             15%. Model-independent limits are derived in single-bin
             signal regions defined by a varying minimum transverse mass
             threshold. The resulting visible cross-section upper limits
             range between 4.6 (15) pb and 22 (22) ab as the threshold
             increases from 130 (110) GeV to 5.1 (5.1) TeV in the
             electron (muon) channel.},
   Doi = {10.1103/PhysRevD.100.052013},
   Key = {fds356572}
}

@article{fds307858,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amoroś, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for a heavy gauge boson decaying to a charged lepton
             and a neutrino in 1 fb-1 of pp collisions at √s
             = 7 TeV using the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {1-2},
   Pages = {28-46},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.09.093},
   Abstract = {The ATLAS detector at the LHC is used to search for
             high-mass states, such as heavy charged gauge bosons (W'),
             decaying to a charged lepton (electron or muon) and a
             neutrino. Results are presented based on the analysis of pp
             collisions at a center-of-mass energy of 7 TeV corresponding
             to an integrated luminosity of 1.04 fb-1. No excess above
             Standard Model expectations is observed. A W' with
             Sequential Standard Model couplings is excluded at the 95%
             confidence level for masses up to 2.15 TeV.},
   Doi = {10.1016/j.physletb.2011.09.093},
   Key = {fds307858}
}

@article{fds356362,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
             C},
   Title = {Search for a heavy Higgs boson decaying into a Z boson and
             another heavy Higgs boson in the ℓℓbb and ℓℓWW final
             states in pp collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {5},
   Year = {2021},
   Month = {May},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09117-5},
   Abstract = {A search for a heavy neutral Higgs boson, A, decaying into a
             Z boson and another heavy Higgs boson, H, is performed using
             a data sample corresponding to an integrated luminosity of
             139 fb- 1 from proton–proton collisions at s=13 TeV
             recorded by the ATLAS detector at the LHC. The search
             considers the Z boson decaying into electrons or muons and
             the H boson into a pair of b-quarks or W bosons. The mass
             range considered is 230–800 GeV for the A boson and
             130–700 GeV for the H boson. The data are in good
             agreement with the background predicted by the Standard
             Model, and therefore 95% confidence-level upper limits for
             σ×B(A→ZH)×B(H→bborH→WW) are set. The upper limits
             are in the range 0.0062–0.380 pb for the H→ bb channel
             and in the range 0.023–8.9 pb for the H→ WW channel. An
             interpretation of the results in the context of
             two-Higgs-doublet models is also given.},
   Doi = {10.1140/epjc/s10052-021-09117-5},
   Key = {fds356362}
}

@article{fds336449,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Arnaez, O and Arnold, H and Arratia, M},
   Title = {Search for a heavy Higgs boson decaying into a Z boson and
             another heavy Higgs boson in the ℓℓbb final state in pp
             collisions at √s= 13 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {783},
   Pages = {392-414},
   Publisher = {Elsevier BV},
   Year = {2018},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.07.006},
   Abstract = {A search for a heavy neutral Higgs boson, A, decaying into a
             Z boson and another heavy Higgs boson, H, is performed using
             a data sample corresponding to an integrated luminosity of
             36.1 fb−1 from proton–proton collisions at s=13 TeV
             recorded in 2015 and 2016 by the ATLAS detector at the Large
             Hadron Collider. The search considers the Z boson decaying
             to electrons or muons and the H boson into a pair of
             b-quarks. No evidence for the production of an A boson is
             found. Considering each production process separately, the
             95% confidence-level upper limits on the pp→A→ZH
             production cross-section times the branching ratio H→bb
             are in the range of 14–830 fb for the gluon–gluon fusion
             process and 26–570 fb for the b-associated process for the
             mass ranges 130–700 GeV of the H boson and 230–800 GeV
             of the A boson. The results are interpreted in the context
             of two-Higgs-doublet models.},
   Doi = {10.1016/j.physletb.2018.07.006},
   Key = {fds336449}
}

@article{fds356787,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for a heavy narrow resonance decaying to eμ eτ or
             μτ with the ATLAS detector in √s=7 TeV pp collisions at
             the LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {723},
   Number = {1-3},
   Pages = {15-32},
   Year = {2013},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.04.035},
   Abstract = {This Letter presents the results of a search for a heavy
             particle decaying into an e±μ∓, e±τ∓, or μ±τ∓
             final state in pp collisions at s=7 TeV. The data were
             recorded with the ATLAS detector at the LHC during 2011 and
             correspond to an integrated luminosity of 4.6 fb−1. No
             significant excess above the Standard Model expectation is
             observed, and exclusions at 95% confidence level are placed
             on the cross section times branching ratio for the
             production of an R-parity-violating supersymmetric tau
             sneutrino. For a sneutrino mass of 500 (2000) GeV, the
             observed limits on the production cross section times
             branching ratio are 3.2 (1.4) fb, 42 (17) fb, and 40 (18) fb
             for the eμ eτ and μτ modes, respectively. These results
             considerably extend constraints from Tevatron
             experiments.},
   Doi = {10.1016/j.physletb.2013.04.035},
   Key = {fds356787}
}

@article{fds310407,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, T and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, A and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D},
   Title = {Search for a heavy neutral particle decaying into an
             electron and a muon using 1 fb-1 of atlas
             data},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {12},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {December},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1809-9},
   Abstract = {A search is presented for a high mass neutral particle that
             decays directly to the e±μ∓ final state. The data sample
             was recorded by the ATLAS detector in √ s = 7 TeV pp
             collisions at the LHC from March to June 2011 and
             corresponds to an integrated luminosity of 1.07 fb-1. The
             data are found to be consistent with the Standard Model
             background. The high e±μ∓ mass region is used to set 95%
             confidence level upper limits on the production of two
             possible new physics processes: tau sneutrinos in an
             R-parity violating supersymmetric model and Z'-like vector
             bosons in a lepton flavor violating model.},
   Doi = {10.1140/epjc/s10052-011-1809-9},
   Key = {fds310407}
}

@article{fds310272,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
             C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
             MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
             N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C and Conti, G},
   Title = {Search for a Heavy Neutral Particle Decaying to eμ, eτ, or
             μτ in pp Collisions at sqrt[s]=8  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {115},
   Number = {3},
   Pages = {031801},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.115.031801},
   Abstract = {This Letter presents a search for a heavy neutral particle
             decaying into an opposite-sign different-flavor dilepton
             pair, e^{±}μ^{∓}, e^{±}τ^{∓}, or μ^{±}τ^{∓}
             using 20.3  fb^{-1} of pp collision data at
             sqrt[s]=8  TeV collected by the ATLAS detector at the
             LHC. The numbers of observed candidate events are compatible
             with the standard model expectations. Limits are set on the
             cross section of new phenomena in two scenarios: the
             production of ν[over ˜]_{τ} in R-parity-violating
             supersymmetric models and the production of a
             lepton-flavor-violating Z^{'} vector boson.},
   Doi = {10.1103/physrevlett.115.031801},
   Key = {fds310272}
}

@article{fds307702,
   Author = {Aaltonen, T and Adelman, J and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
             W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Rao, K and Redondo, I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Search for a heavy particle decaying to a top quark and a
             light quark in pp ¯ collisions at √s=1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {21},
   Pages = {211805},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.211805},
   Abstract = {We present a search for a new heavy particle X produced in
             association with a top quark, pp[over ¯]→t(X→t[over
             ¯]q) or pp[over ¯]→t[over ¯](X[over ¯]→tq[over ¯]),
             where q stands for up quarks and down quarks. Such a
             particle may explain the recent anomalous measurements of
             top-quark forward-backward asymmetry. If the light-flavor
             quark (q) is reconstructed as a jet (j), this gives a t[over
             ¯]+j or t+j resonance in tt[over ¯]+jet events, a
             previously unexplored experimental signature. In a sample of
             events with exactly one lepton, missing transverse momentum
             and at least five jets, corresponding to an integrated
             luminosity of 8.7 fb(-1) collected by the CDF II detector,
             we find the data to be consistent with the standard model.
             We set cross-section upper limits on the production (pp[over
             ¯]→Xt or X[over ¯]t[over ¯]) at 95% confidence level
             from 0.61 pb to 0.02 pb for X masses ranging from 200
             GeV/c(2) to 800 GeV/c(2), respectively.},
   Doi = {10.1103/physrevlett.108.211805},
   Key = {fds307702}
}

@article{fds307748,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {Search for a heavy Standard Model Higgs boson in the channel
             H→ZZ→ℓ+-qq̄ using the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {707},
   Number = {1},
   Pages = {27-45},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.11.056},
   Abstract = {A search for a heavy Standard Model Higgs boson decaying via
             H→ZZ→ℓ+ℓ-qq̄, where ℓ=e, μ, is presented. The
             search is performed using a data set of pp collisions at
             √s=7 TeV, corresponding to an integrated luminosity of
             1.04 fb-1 collected in 2011 by the ATLAS detector at the
             CERN LHC collider. No significant excess of events above the
             estimated background is found. Upper limits at 95%
             confidence level on the production cross section (relative
             to that expected from the Standard Model) of a Higgs boson
             with a mass in the range between 200 and 600 GeV are
             derived. Within this mass range, there is at present
             insufficient sensitivity to exclude a Standard Model Higgs
             boson. For a Higgs boson with a mass of 360 GeV, where the
             sensitivity is maximal, the observed and expected cross
             section upper limits are factors of 1.7 and 2.7,
             respectively, larger than the Standard Model prediction. ©
             2011 CERN.},
   Doi = {10.1016/j.physletb.2011.11.056},
   Key = {fds307748}
}

@article{fds320776,
   Author = {ATLAS Collaboration},
   Title = {Search for a heavy top-quark partner in final states with
             two leptons with the ATLAS detector at the
             LHC},
   Journal = {JHEP},
   Volume = {1211},
   Number = {11},
   Pages = {094},
   Publisher = {Springer Nature},
   Year = {2012},
   url = {http://dx.doi.org/10.1007/JHEP11(2012)094},
   Abstract = {http://dx.doi.org/10.1007/JHEP11(2012)094},
   Doi = {10.1007/JHEP11(2012)094},
   Key = {fds320776}
}

@article{fds307828,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De
             Cecco, S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier,
             L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
             R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
             S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis,
             E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu,
             T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck,
             J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak,
             R and Maeshima, K and Makhoul, K and Maksimovic, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez,
             T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Santi,
             L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt,
             M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki,
             M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
             P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner,
             RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters,
             D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK},
   Title = {Search for a heavy toplike quark in pp collisions at
             √s=1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {107},
   Number = {26},
   Pages = {261801},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.107.261801},
   Abstract = {We present the results of a search for pair production of a
             heavy toplike (t') quark decaying to Wq final states using
             data corresponding to an integrated luminosity of 5.6 fb(-1)
             collected by the CDF II detector in pp collisions at
             √s=1.96 TeV. We perform parallel searches for t'→Wb and
             t'→Wq (where q is a generic down-type quark) in events
             containing a lepton and four or more jets. By performing a
             fit to the two-dimensional distribution of total transverse
             energy versus reconstructed t' quark mass, we set upper
             limits on the t't' production cross section and exclude a
             standard model fourth-generation t' quark decaying to Wb
             (Wq) with mass below 358 (340) GeV/c(2) at 95%
             C.L.},
   Doi = {10.1103/physrevlett.107.261801},
   Key = {fds307828}
}

@article{fds307658,
   Author = {Aaltonen, T and Adelman, J and Lvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
             W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F},
   Title = {Search for a heavy vector boson decaying to two gluons in
             pp̄ collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.112002},
   Abstract = {We present a search for a new heavy vector boson Z′ that
             decays to gluons. Decays to on-shell gluons are suppressed,
             leading to a dominant decay mode of Z′→g*g. We study the
             case where the off-shell gluon g* converts to a pair of top
             quarks, leading to a final state of tt̄g. In a sample of
             events with exactly one charged lepton, large missing
             transverse momentum and at least five jets, corresponding to
             an integrated luminosity of 8.7fb-1 collected by the CDF II
             detector, we find the data to be consistent with the
             standard model. We set upper limits on the production cross
             section times branching ratio of this chromophilic Z′ at
             95% confidence level from 300 to 40 fb for Z′ masses
             ranging from 400 to 1000GeV/c2, respectively. © 2012
             American Physical Society.},
   Doi = {10.1103/PhysRevD.86.112002},
   Key = {fds307658}
}

@article{fds307964,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
             A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
             A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey,
             P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni, GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes,
             D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani,
             M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
             S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo,
             KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin,
             PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko,
             S and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen,
             AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Movilla Fernandez and P and Mülmenstädt,
             J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura,
             K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman,
             M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Griso, SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino,
             G and Pianori, E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
             J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Rekovic, V and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Saltó,
             O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro,
             A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker,
             GL},
   Title = {Search for a Higgs boson decaying to two W bosons at
             CDF.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {2},
   Pages = {021802},
   Year = {2009},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.102.021802},
   Abstract = {We present a search for a Higgs boson decaying to two W
             bosons in pp[over ] collisions at sqrt[s]=1.96 TeV
             center-of-mass energy. The data sample corresponds to an
             integrated luminosity of 3.0 fb;(-1) collected with the CDF
             II detector. We find no evidence for production of a Higgs
             boson with mass between 110 and 200 GeV/c;(2), and determine
             upper limits on the production cross section. For the mass
             of 160 GeV/c;(2), where the analysis is most sensitive, the
             observed (expected) limit is 0.7 pb (0.9 pb) at 95% Bayesian
             credibility level which is 1.7 (2.2) times the standard
             model cross section.},
   Doi = {10.1103/physrevlett.102.021802},
   Key = {fds307964}
}

@article{fds307716,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
             M and de Barbaro, P and De Cecco and S and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
             G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
             JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
             K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
             M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker,
             A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
             E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Ray, J and Redondo, I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro,
             A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri,
             F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari,
             M and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton,
             O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov,
             A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK},
   Title = {Search for a Higgs boson in the diphoton final state in pp
             collisions at sqrt[s]=1.96  TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {1},
   Pages = {011801},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.108.011801},
   Abstract = {A search for a narrow Higgs boson resonance in the diphoton
             mass spectrum is presented based on data corresponding to
             7.0  fb{-1} of integrated luminosity from pp collisions
             at sqrt[s]=1.96  TeV collected by the CDF experiment. No
             evidence of such a resonance is observed, and upper limits
             are set on the cross section times branching ratio of the
             resonant state as a function of Higgs boson mass. The limits
             are interpreted in the context of the standard model and one
             fermiophobic benchmark model where the data exclude
             fermiophobic Higgs bosons with masses below
             114  GeV/c{2} at a 95% Bayesian credibility
             level.},
   Doi = {10.1103/physrevlett.108.011801},
   Key = {fds307716}
}

@article{fds307681,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M},
   Title = {Search for a Higgs boson in the diphoton final state using
             the full CDF data set from pp collisions at
             s=1.96TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {717},
   Number = {1-3},
   Pages = {173-181},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.08.051},
   Abstract = {A search for a narrow Higgs boson resonance in the diphoton
             mass spectrum is presented based on data corresponding to
             10fb -1 of integrated luminosity collected by the CDF
             experiment from proton-antiproton collisions at s=1.96TeV.
             To increase the sensitivity of the search, we employ a
             multivariate discriminant technique for the first time in
             this channel at CDF. No evidence of signal is observed, and
             upper limits are set on the cross section times branching
             ratio of the resonant state as a function of the Higgs boson
             mass. The limits are interpreted in the context of the
             standard model with an expected (observed) limit on the
             cross section times branching ratio of 9.9 (17.0) times the
             standard model prediction at the 95% credibility level for a
             Higgs boson mass of 125GeV/c 2. Moreover, a Higgs boson with
             suppressed couplings to fermions is excluded for masses
             below 114GeV/c 2 at the 95% credibility level. © 2012
             Elsevier B.V.},
   Doi = {10.1016/j.physletb.2012.08.051},
   Key = {fds307681}
}

@article{fds308051,
   Author = {Aaltonen, and T, and others},
   Title = {Search for a high-mass diphoton state and limits on
             Randall-Sundrum gravitons at CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {17},
   Pages = {171801},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.99.171801},
   Abstract = {e have performed a search for new particles which decay to
             two photons using 1.2 fb-1 of integrated luminosity from
             p[overline p] collisions at sqrt(s)=1.96 TeV collected using
             the CDF II detector at the Fermilab Tevatron. We find the
             diphoton mass spectrum to be in agreement with the standard
             model expectation, and set limits on the cross section times
             branching ratio for the Randall-Sundrum graviton, as a
             function of diphoton mass. We subsequently derive lower
             limits for the graviton mass of 230 GeV/c2 and 850 GeV/c2,
             at the 95\% confidence level, for coupling parameters
             (k/[overline M]Pl) of 0.01 and 0.1, respectively.},
   Doi = {10.1103/physrevlett.99.171801},
   Key = {fds308051}
}

@article{fds356786,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for a high-mass Higgs boson decaying to a W boson
             pair in pp collisions at (Formula presented.) TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {1},
   Pages = {1-66},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2016)032},
   Abstract = {Abstract: A search for a high-mass Higgs boson H is
             performed in the H → WW → ℓνℓν and H → WW →
             ℓνqq decay channels using pp collision data corresponding
             to an integrated luminosity of 20.3 fb−1 collected at
             s=8(Formula presented.) TeV by the ATLAS detector at the
             Large Hadron Collider. No evidence of a high-mass Higgs
             boson is found. Limits on σH × BR(H → WW) as a function
             of the Higgs boson mass mH are determined in three different
             scenarios: one in which the heavy Higgs boson has a narrow
             width compared to the experimental resolution, one for a
             width increasing with the boson mass and modeled by the
             complex-pole scheme following the same behavior as in the
             Standard Model, and one for intermediate widths. The upper
             range of the search is mH = 1500 GeV for the narrow-width
             scenario and mH = 1000 GeV for the other two scenarios. The
             lower edge of the search range is 200–300 GeV and depends
             on the analysis channel and search scenario. For each signal
             interpretation, individual and combined limits from the two
             WW decay channels are presented. At mH = 1500 GeV, the
             highest-mass point tested, σH × BR(H → WW) for a
             narrow-width Higgs boson is constrained to be less than 22
             fb and 6.6 fb at 95% CL for the gluon fusion and
             vector-boson fusion production modes, respectively.[Figure
             not available: see fulltext.]},
   Doi = {10.1007/JHEP01(2016)032},
   Key = {fds356786}
}

@article{fds307600,
   Author = {The ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
             M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asner, D and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu,
             E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt,
             J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y},
   Title = {Search for a light charged Higgs boson in the decay channel
             [Formula: see text] in [Formula: see text] events using
             pp collisions at [Formula: see text] with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {6},
   Pages = {2465},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2465-z},
   Abstract = {A search for a charged Higgs boson (<i>H</i><sup>+</sup>) in
             [Formula: see text] decays is presented, where one of the
             top quarks decays via <i>t</i>→<i>H</i><sup>+</sup><i>b</i>,
             followed by <i>H</i><sup>+</sup>→ two jets ([Formula: see
             text]). The other top quark decays to <i>Wb</i>, where the
             <i>W</i> boson then decays into a lepton
             (<i>e</i>/<i>μ</i>) and a neutrino. The data were recorded
             in <i>pp</i> collisions at [Formula: see text] by the ATLAS
             detector at the LHC in 2011, and correspond to an integrated
             luminosity of 4.7 fb<sup>-1</sup>. With no observation of a
             signal, 95 % confidence level (CL) upper limits are set on
             the decay branching ratio of top quarks to charged Higgs
             bosons varying between 5 % and 1 % for
             <i>H</i><sup>+</sup> masses between 90 GeV and 150 GeV,
             assuming [Formula: see text].},
   Doi = {10.1140/epjc/s10052-013-2465-z},
   Key = {fds307600}
}

@article{fds307698,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten,
             K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
             Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau,
             T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B},
   Title = {Search for a light Higgs boson decaying to long-lived weakly
             interacting particles in proton-proton collisions at sqrt[s]
             = 7 TeV with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {25},
   Pages = {251801},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.108.251801},
   Abstract = {A search for the decay of a light Higgs boson (120-140 GeV)
             to a pair of weakly interacting, long-lived particles in
             1.94 fb(-1) of proton-proton collisions at sqrt[s] = 7 TeV
             recorded in 2011 by the ATLAS detector is presented. The
             search strategy requires that both long-lived particles
             decay inside the muon spectrometer. No excess of events is
             observed above the expected background and limits on the
             Higgs boson production times branching ratio to weakly
             interacting, long-lived particles are derived as a function
             of the particle proper decay length.},
   Doi = {10.1103/physrevlett.108.251801},
   Key = {fds307698}
}

@article{fds321119,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Erbacher, R and Errede, S and Esham,
             B},
   Title = {Search for a low-mass neutral Higgs boson with suppressed
             couplings to fermions using events with multiphoton final
             states},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.112010},
   Abstract = {A search for a Higgs boson with suppressed couplings to
             fermions, hf, assumed to be the neutral, lower-mass partner
             of the Higgs boson discovered at the Large Hadron Collider,
             is reported. Such a Higgs boson could exist in extensions of
             the standard model with two Higgs doublets, and could be
             produced via pp→H±hf→W∗hfhf→4γ+X, where H± is a
             charged Higgs boson. This analysis uses all events with at
             least three photons in the final state from
             proton-antiproton collisions at a center-of-mass energy of
             1.96 TeV collected by the Collider Detector at Fermilab,
             corresponding to an integrated luminosity of 9.2 fb-1. No
             evidence of a signal is observed in the data. Values of
             Higgs-boson masses between 10 and 100 GeV/c2 are excluded at
             95% Bayesian credibility.},
   Doi = {10.1103/PhysRevD.93.112010},
   Key = {fds321119}
}

@article{fds307707,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar,
             C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De Cecco and S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
             G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
             JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
             K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
             M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker,
             A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee,
             E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro,
             P and Makhoul, K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín,
             R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
             P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán,
             J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang,
             T},
   Title = {Search for a low-mass standard model Higgs boson in the ττ
             decay channel in pp collisions at sqrt[s]=1.96  TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {18},
   Pages = {181804},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.181804},
   Abstract = {We report on a search for the standard model Higgs boson
             decaying into pairs of τ leptons in pp collisions produced
             by the Tevatron at sqrt[s]=1.96  TeV. The analyzed data
             sample was recorded by the CDFII detector and corresponds to
             an integrated luminosity of 6.0  fb(-1). The search is
             performed in the final state with one τ decaying
             leptonically and the second one identified through its
             semihadronic decay. Since no significant excess is observed,
             a 95% credibility level upper limit on the production cross
             section times branching ratio to the ττ final state is set
             for hypothetical Higgs boson masses between 100 and
             150  GeV/c2. For a Higgs boson of 120  GeV/c2 the
             observed (expected) limit is 14.6 (15.3) the predicted
             value.},
   Doi = {10.1103/physrevlett.108.181804},
   Key = {fds307707}
}

@article{fds307550,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin,
             JF},
   Title = {Search for a multi-Higgs-boson cascade in W+W
             -bb̄ events with the ATLAS detector in pp
             collisions at √s = 8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.032002},
   Abstract = {A search is presented for new particles in an extension to
             the Standard Model that includes a heavy Higgs boson (H0),
             an intermediate charged Higgs-boson pair (H-), and a light
             Higgs boson (h0). The analysis searches for events involving
             the production of a single heavy neutral Higgs boson which
             decays to the charged Higgs boson and a W boson, where the
             charged Higgs boson subsequently decays into a W boson and
             the lightest neutral Higgs boson decaying to a
             bottom-antibottom-quark pair. Such a cascade results in a
             W-boson pair and a bottom-antibottom-quark pair in the final
             state. Events with exactly one lepton, missing transverse
             momentum, and at least four jets are selected from a data
             sample corresponding to an integrated luminosity of 20.3
             fb-1, collected by the ATLAS detector in proton-proton
             collisions at √s = 8 TeV at the LHC. The data are found to
             be consistent with Standard Model predictions, and 95%
             confidence-level upper limits are set on the product of
             cross section and branching ratio. These limits range from
             0.065 to 43 pb as a function of H0 and H- masses, with mh0
             fixed at 125 GeV. © 2014 CERN, for the ATLAS
             Collaboration.},
   Doi = {10.1103/PhysRevD.89.032002},
   Key = {fds307550}
}

@article{fds308089,
   Author = {Abulencia, and A, and others},
   Title = {Search for a neutral Higgs boson decaying to a W boson pair
             in $p\bar{p}$ collisions at $\sqrt{s} =$
             1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {97},
   Number = {8},
   Pages = {081802},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.97.081802},
   Abstract = {We present the results of a search for standard model Higgs
             boson production with decay to WW*, identified through the
             leptonic final states e+e-nu-bar nu, e+/- mu-/+ nu-bar nu
             and mu+ mu- nu-bar nu. This search uses 360 pb-1 of data
             collected from p anti-p collisions at s**(1/2) = 1.96 TeV by
             the upgraded Collider Detector at Fermilab (CDF II). We
             observe no signal excess and set 95% confidence level upper
             limits on the production cross section times branching ratio
             for the Higgs boson to WW* or any new scalar particle with
             similar decay products. These upper limits range from 5.5 to
             3.2 pb for Higgs boson masses between 120 and 200
             GeV/c2.},
   Doi = {10.1103/physrevlett.97.081802},
   Key = {fds308089}
}

@article{fds307882,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for a new heavy gauge boson ${W}^{$'${}}$ with event
             signature $\mathrm{\text{electron}}+\mathrm{\text{missing}}$
             transverse energy in $p\overline{p}$ collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {3},
   Pages = {031102},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.031102},
   Abstract = {We present a search for a new heavy charged vector boson
             W′ decaying to an electron-neutrino pair in pp̄
             collisions at a center-of-mass energy of 1.96 TeV. The data
             were collected with the CDF II detector and correspond to an
             integrated luminosity of 5.3fb-1. No significant excess
             above the standard model expectation is observed and we set
             upper limits on σ•B(W′→eν). Assuming standard model
             couplings to fermions and the neutrino from the W′ boson
             decay to be light, we exclude a W′ boson with mass less
             than 1.12TeV/c2 at the 95% confidence level. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.83.031102},
   Key = {fds307882}
}

@article{fds347476,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines,
             JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann,
             TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
             NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
             TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ},
   Title = {Search for a new heavy gauge-boson resonance decaying into a
             lepton and missing transverse momentum in 36 fb - 1 of
             pp collisions at s = 13  TeV with the ATLAS
             experiment.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {5},
   Pages = {401},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-5877-y},
   Abstract = {The results of a search for new heavy W ' bosons decaying to
             an electron or muon and a neutrino using proton-proton
             collision data at a centre-of-mass energy of s = 13  TeV
             are presented. The dataset was collected in 2015 and 2016 by
             the ATLAS experiment at the Large Hadron Collider and
             corresponds to an integrated luminosity of 36.1  fb - 1 .
             As no excess of events above the Standard Model prediction
             is observed, the results are used to set upper limits on the
             W ' boson cross-section times branching ratio to an electron
             or muon and a neutrino as a function of the W ' mass.
             Assuming a W ' boson with the same couplings as the Standard
             Model <i>W</i> boson, W ' masses below 5.1 TeV are excluded
             at the 95% confidence level.},
   Doi = {10.1140/epjc/s10052-018-5877-y},
   Key = {fds347476}
}

@article{fds375228,
   Author = {Filmer, EK and Jackson, P and Kong, AXY and Pandya, HD and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Castillo, FL and Costanza, F and Delmastro, M and Di
             Ciaccio, L and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo
             Martinez, N and Poddar, G and Sanchez Pineda and A and Sauvan, E and Bernardi, G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Li, T and Marchiori, G and Nakkalil, K and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
             Gemmeren, P and Wamorkar, T and Wang, R and Zhang, J and Cheu, E and Cui,
             Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Tost,
             M},
   Title = {Search for a new pseudoscalar decaying into a pair of muons
             in events with a top-quark pair at Formula Presented with
             the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {108},
   Number = {9},
   Year = {2023},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.108.092007},
   Abstract = {A search for a new pseudoscalar Formula Presented-boson
             produced in events with a top-quark pair, where the Formula
             Presented-boson decays into a pair of muons, is performed
             using Formula Presented Formula Presented collision data
             collected with the ATLAS detector at the LHC, corresponding
             to an integrated luminosity of Formula Presented. The search
             targets the final state where only one top quark decays to
             an electron or muon, resulting in a signature with three
             leptons Formula Presented and Formula Presented. No
             significant excess of events above the Standard Model
             expectation is observed and upper limits are set on two
             signal models: Formula Presented and Formula Presented with
             Formula Presented, Formula Presented, where Formula
             Presented, in the mass ranges Formula Presented and Formula
             Presented.},
   Doi = {10.1103/PhysRevD.108.092007},
   Key = {fds375228}
}

@article{fds313593,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Beven, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM},
   Title = {Search for a new resonance decaying to a W or
             Z boson and a Higgs boson in the [Formula: see text]
             final states with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {6},
   Pages = {263},
   Year = {2015},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3474-x},
   Abstract = {A search for a new resonance decaying to a <i>W</i> or
             <i>Z</i> boson and a Higgs boson in the [Formula: see text]
             final states is performed using 20.3 fb[Formula: see text]
             of <i>pp</i> collision data recorded at [Formula: see
             text] 8 TeV with the ATLAS detector at the Large Hadron
             Collider. The search is conducted by examining the
             <i>WH</i> / <i>ZH</i> invariant mass distribution for a
             localized excess. No significant deviation from the Standard
             Model background prediction is observed. The results are
             interpreted in terms of constraints on the Minimal Walking
             Technicolor model and on a simplified approach based on a
             phenomenological Lagrangian of Heavy Vector
             Triplets.},
   Doi = {10.1140/epjc/s10052-015-3474-x},
   Key = {fds313593}
}

@article{fds356559,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
             Abud, A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid,
             OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios,
             C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras,
             D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella,
             L},
   Title = {Search for a right-handed gauge boson decaying into a
             high-momentum heavy neutrino and a charged lepton in pp
             collisions with the ATLAS detector at s=13
             TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {798},
   Year = {2019},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.134942},
   Abstract = {A search for a right-handed gauge boson WR, decaying into a
             boosted right-handed heavy neutrino NR, in the framework of
             Left-Right Symmetric Models is presented. It is based on
             data from proton–proton collisions with a centre-of-mass
             energy of 13 TeV collected by the ATLAS detector at the
             Large Hadron Collider during the years 2015, 2016 and 2017,
             corresponding to an integrated luminosity of 80 fb−1. The
             search is performed separately for electrons and muons in
             the final state. A distinguishing feature of the search is
             the use of large-radius jets containing electrons.
             Selections based on the signal topology result in smaller
             background compared to the expected signal. No significant
             deviation from the Standard Model prediction is observed and
             lower limits are set in the WR and NR mass plane. Mass
             values of the WR smaller than 3.8–5 TeV are excluded for
             NR in the mass range 0.1–1.8 TeV.},
   Doi = {10.1016/j.physletb.2019.134942},
   Key = {fds356559}
}

@article{fds352202,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C},
   Title = {Search for a scalar partner of the top quark in the
             all-hadronic tt¯ plus missing transverse momentum final
             state at √s=13 TeV with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {8},
   Year = {2020},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-8102-8},
   Abstract = {A search for direct pair production of scalar partners of
             the top quark (top squarks or scalar third-generation
             up-type leptoquarks) in the all-hadronic tt¯ plus missing
             transverse momentum final state is presented. The analysis
             of 139 fb - 1 of s=13 TeV proton–proton collision data
             collected using the ATLAS detector at the LHC yields no
             significant excess over the Standard Model background
             expectation. To interpret the results, a supersymmetric
             model is used where the top squark decays via
             t~→t(∗)χ~10, with t(∗) denoting an on-shell
             (off-shell) top quark and χ~10 the lightest neutralino.
             Three specific event selections are optimised for the
             following scenarios. In the scenario where mt~>mt+mχ~10,
             top squark masses are excluded in the range 400–1250 GeV
             for χ~10 masses below 200 GeV at 95% confidence level. In
             the situation where mt~∼mt+mχ~10, top squark masses in
             the range 300–630 GeV are excluded, while in the case
             where mt~<mW+mb+mχ~10 (with mt~-mχ~10≥5 GeV),
             considered for the first time in an ATLAS all-hadronic
             search, top squark masses in the range 300–660 GeV are
             excluded. Limits are also set for scalar third-generation
             up-type leptoquarks, excluding leptoquarks with masses below
             1240 GeV when considering only leptoquark decays into a top
             quark and a neutrino.},
   Doi = {10.1140/epjc/s10052-020-8102-8},
   Key = {fds352202}
}

@article{fds356719,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Search for a scalar partner of the top quark in the jets
             plus missing transverse momentum final state at √s=13 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {12},
   Year = {2017},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2017)085},
   Abstract = {A search for pair production of a scalar partner of the top
             quark in events with four or more jets plus missing
             transverse momentum is presented. An analysis of 36.1 fb−1
             of s=13 TeV proton-proton collisions collected using the
             ATLAS detector at the LHC yields no significant excess over
             the expected Standard Model background. To interpret the
             results a simplified supersymmetric model is used where the
             top squark is assumed to decay via t˜1→t(∗)χ˜10 and
             t˜1→bχ˜1±→bW(∗)χ˜10, where χ10(χ1±) denotes
             the lightest neutralino (chargino). Exclusion limits are
             placed in terms of the top-squark and neutralino masses.
             Assuming a branching ratio of 100% to tχ˜10, top-squark
             masses in the range 450–1000 GeV are excluded for χ˜10
             masses below 160 GeV. In the case where mt˜1∼mt+mχ˜10,
             top-squark masses in the range 235–590 GeV are
             excluded.},
   Doi = {10.1007/JHEP12(2017)085},
   Key = {fds356719}
}

@article{fds307832,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
             G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
             M and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius,
             C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG},
   Title = {Search for a standard model Higgs boson in the
             H→ZZ→ℓ(+)ℓ(-)νν decay channel with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {107},
   Number = {22},
   Pages = {221802},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.107.221802},
   Abstract = {A search for a heavy standard model Higgs boson decaying via
             H→ZZ→→ℓ(+)ℓ(-)νν, where ℓ=e, μ, is presented.
             It is based on proton-proton collision data at √s=7 TeV,
             collected by the ATLAS experiment at the LHC in the first
             half of 2011 and corresponding to an integrated luminosity
             of 1.04 fb(-1). The data are compared to the expected
             standard model backgrounds. The data and the background
             expectations are found to be in agreement and upper limits
             are placed on the Higgs boson production cross section over
             the entire mass window considered; in particular, the
             production of a standard model Higgs boson is excluded in
             the region 340<m(H)<450 GeV at the 95% confidence
             level.},
   Doi = {10.1103/physrevlett.107.221802},
   Key = {fds307832}
}

@article{fds307795,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D},
   Title = {Search for a standard model Higgs boson in the
             H→ZZ→ℓ+νν¯ decay
             channel using 4.7 fb−1 of √s=7 TeV data with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {717},
   Number = {1-3},
   Pages = {29-48},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {October},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.09.016},
   Abstract = {A search for a Standard Model Higgs boson decaying via
             H→ZZ→ℓ+ℓ−νν¯ where ℓ represents electrons or
             muons, is presented. It is based on proton-proton collision
             data at s=7 TeV, collected by the ATLAS experiment at the
             LHC during 2011 and corresponding to an integrated
             luminosity of 4.7 fb−1. The data agree with the expected
             Standard Model backgrounds. Upper limits on the Higgs boson
             production cross section are derived for Higgs boson masses
             between 200 GeV and 600 GeV and the production of a Standard
             Model Higgs boson with a mass in the range 319–558 GeV is
             excluded at the 95% confidence level.},
   Doi = {10.1016/j.physletb.2012.09.016},
   Key = {fds307795}
}

@article{fds307785,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel,
             M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
             M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
             T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins,
             NJ and Collins-Tooth, C and Collot, J and Colombo,
             T},
   Title = {Search for a Standard Model Higgs boson in the mass range
             200-600GeV in the H→ZZ→ℓ+ℓ-qq̄ decay channel with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {717},
   Number = {1-3},
   Pages = {70-88},
   Publisher = {Elsevier BV},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.09.020},
   Abstract = {A search for a heavy Standard Model Higgs boson decaying via
             H→ZZ→ℓ+ℓ-qq̄, where ℓ=e or μ, is presented. The
             search uses a data set of pp collisions at s=7TeV,
             corresponding to an integrated luminosity of 4.7fb-1
             collected in 2011 by the ATLAS detector at the CERN LHC. No
             significant excess of events above the estimated background
             is found. Upper limits at 95% confidence level on the
             production cross section of a Higgs boson with a mass in the
             range between 200 and 600GeV are derived. A Standard Model
             Higgs boson with a mass in the range 300GeV≤mH≤322GeV or
             353GeV≤mH≤410GeV is excluded at 95% CL. The
             corresponding expected exclusion range is
             351GeV≤mH≤404GeV at 95% CL. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.09.020},
   Key = {fds307785}
}

@article{fds307942,
   Author = {Aaltonen, T and others},
   Title = {Search for a Standard Model Higgs Boson in WH→ℓvbb̅ in
             pp̅ Collisions at sqrt[s] =1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {10},
   Pages = {101802},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.101802},
   Abstract = {We present a search for a standard model Higgs boson
             produced in association with a W boson using 2.7  fb-1
             of integrated luminosity of pp̅ collision data taken at
             sqrt[s]=1.96  TeV. Limits on the Higgs boson production
             rate are obtained for masses between 100 and
             150  GeV/c2. Through the use of multivariate techniques,
             the analysis achieves an observed (expected) 95% confidence
             level upper limit of 5.6 (4.8) times the theoretically
             expected production cross section for a standard model Higgs
             boson with a mass of 115  GeV/c2.},
   Doi = {10.1103/physrevlett.103.101802},
   Key = {fds307942}
}

@article{fds347460,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
             P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
             H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Bakshi
             Gupta, D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
             NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
             AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov,
             A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin,
             DL and Bristow, TM and Britton, D and Britzger, D and Brock, I and Brock,
             R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni,
             A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
             MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard,
             CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
             R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
             JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran,
             J},
   Title = {Search for a Structure in the B_{s}^{0}π^{±} Invariant
             Mass Spectrum with the ATLAS Experiment.},
   Journal = {Physical review letters},
   Volume = {120},
   Number = {20},
   Pages = {202007},
   Year = {2018},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.120.202007},
   Abstract = {A search for the narrow structure, X(5568), reported by the
             D0 Collaboration in the decay sequence X→B_{s}^{0}π^{±},
             B_{s}^{0}→J/ψϕ, is presented. The analysis is based on a
             data sample recorded with the ATLAS detector at the LHC
             corresponding to 4.9  fb^{-1} of pp collisions at 7 TeV
             and 19.5  fb^{-1} at 8 TeV. No significant signal was
             found. Upper limits on the number of signal events, with
             properties corresponding to those reported by D0, and on the
             X production rate relative to B_{s}^{0} mesons, ρ_{X}, were
             determined at 95% confidence level. The results are
             N(X)<382 and ρ_{X}<0.015 for B_{s}^{0} mesons with
             transverse momenta above 10 GeV, and N(X)<356 and
             ρ_{X}<0.016 for transverse momenta above 15 GeV. Limits
             are also set for potential B_{s}^{0}π^{±} resonances in
             the mass range 5550 to 5700 MeV.},
   Doi = {10.1103/physrevlett.120.202007},
   Key = {fds347460}
}

@article{fds307666,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer,
             F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
             Harpaz, S and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov,
             O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Search for a supersymmetric partner to the top quark in
             final states with jets and missing transverse momentum at
             sqrt[s] = 7 TeV with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {21},
   Pages = {211802},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.109.211802},
   Abstract = {A search for direct pair production of supersymmetric top
             squarks (t(1)) is presented, assuming the t(1) decays into a
             top quark and the lightest supersymmetric particle,
             χ(1)(0), and that both top quarks decay to purely hadronic
             final states. A total of 16 (4) events are observed compared
             to a predicted standard model background of
             13.5(-3.6)(+3.7)(4.4(-1.3)(+1.7)) events in two signal
             regions based on ∫Ldt = 4.7 fb(-1) of pp collision data
             taken at sqrt[s] = 7 TeV with the ATLAS detector at the LHC.
             An exclusion region in the t(1) versus χ(1)(0) mass plane
             is evaluated: 370<m(t)(1)}<465 GeV is excluded for
             m(χ)(1)(0) ~ 0 GeV while m(t)(1) = 445 GeV is excluded for
             m(χ)(1)(0) ≤ 50 GeV.},
   Doi = {10.1103/physrevlett.109.211802},
   Key = {fds307666}
}

@article{fds307609,
   Author = {Aaltonen, T and Adelman, J and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
             W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Johnstone, A and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Rao, K and Redondo, I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Truong, A and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund,
             AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson,
             JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Search for a two-Higgs-boson doublet using a simplified
             model in pp collisions at sqrt[s] = 1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {12},
   Pages = {121801},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.110.121801},
   Abstract = {We present a search for new particles in an extension to the
             standard model that includes a heavy Higgs boson (H(0)), a
             lighter charged Higgs boson (H(±)), and an even lighter
             Higgs boson h(0), with decays leading to a W-boson pair and
             a bottom-antibottom quark pair in the final state. We use
             events with exactly one lepton, missing transverse momentum,
             and at least four jets in data corresponding to an
             integrated luminosity of 8.7 fb(-1) collected by the CDF II
             detector in proton-antiproton collisions at sqrt[s]= 1.96
             TeV. We find the data to be consistent with standard model
             predictions and report the results in terms of a simplified
             Higgs-cascade-decay model, setting 95% confidence level
             upper limits on the product of cross section and branching
             fraction from 1.3 pb to 15 fb as a function of H(0) and
             H(±) masses for m(h)(0) = 126 GeV/c(2).},
   Doi = {10.1103/physrevlett.110.121801},
   Key = {fds307609}
}

@article{fds307844,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for a Very Light ${CP}$-Odd {H}iggs Boson in Top
             Quark Decays from $p\overline{p}$ Collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {3},
   Pages = {031801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.031801},
   Abstract = {We present the results of a search for a very light CP-odd
             Higgs boson a(1)(0) originating from top quark decays t →
             H(±)b → W(±(*)) a(1)(0)b, and subsequently decaying into
             τ+ τ-. Using a data sample corresponding to an integrated
             luminosity of 2.7  fb(-1) collected by the CDF II
             detector in pp collisions at 1.96 TeV, we perform a search
             for events containing a lepton, three or more jets, and an
             additional isolated track with transverse momentum in the
             range 3 to 20  GeV/c. Observed events are consistent
             with background sources, and 95% C.L. limits are set on the
             branching ratio of t → H(±)b for various masses of H(±)
             and a(1)(0).},
   Doi = {10.1103/PhysRevLett.107.031801},
   Key = {fds307844}
}

@article{fds356702,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for additional heavy neutral Higgs and gauge bosons
             in the ditau final state produced in 36 fb−1 of
             pp collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {1},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2018)055},
   Abstract = {A search for heavy neutral Higgs bosons and Z′ bosons is
             performed using a data sample corresponding to an integrated
             luminosity of 36.1 fb−1 from proton-proton collisions at
             s=13 TeV recorded by the ATLAS detector at the LHC during
             2015 and 2016. The heavy resonance is assumed to decay to
             τ+τ− with at least one tau lepton decaying to final
             states with hadrons and a neutrino. The search is performed
             in the mass range of 0.2-2.25 TeV for Higgs bosons and
             0.2-4.0 TeV for Z′ bosons. The data are in good agreement
             with the background predicted by the Standard Model. The
             results are interpreted in benchmark scenarios. In the
             context of the hMSSM scenario, the data exclude tan β > 1.0
             for mA = 0.25 TeV and tan β > 42 for mA = 1.5 TeV at the
             95% confidence level. For the Sequential Standard Model,
             ZSSM′ with mZ′ < 2.42 TeV is excluded at 95% confidence
             level, while ZNU′ with mZ ′ < 2.25 TeV is excluded for
             the non-universal G(221) model that exhibits enhanced
             couplings to third-generation fermions.},
   Doi = {10.1007/JHEP01(2018)055},
   Key = {fds356702}
}

@article{fds321129,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
             J},
   Title = {Search for an additional, heavy Higgs boson in the [Formula:
             see text] decay channel at [Formula: see text] in [Formula:
             see text] collision data with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {45},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3820-z},
   Abstract = {A search is presented for a high-mass Higgs boson in the
             [Formula: see text], [Formula: see text], [Formula: see
             text], and [Formula: see text] decay modes using the ATLAS
             detector at the CERN Large Hadron Collider. The search uses
             proton-proton collision data at a centre-of-mass energy of
             8 TeV corresponding to an integrated luminosity of
             20.3 fb[Formula: see text]. The results of the search are
             interpreted in the scenario of a heavy Higgs boson with a
             width that is small compared with the experimental mass
             resolution. The Higgs boson mass range considered extends up
             to [Formula: see text] for all four decay modes and down to
             as low as 140 [Formula: see text], depending on the decay
             mode. No significant excess of events over the Standard
             Model prediction is found. A simultaneous fit to the four
             decay modes yields upper limits on the production
             cross-section of a heavy Higgs boson times the branching
             ratio to [Formula: see text] boson pairs. 95 % confidence
             level upper limits range from 0.53 pb at [Formula: see
             text] GeV to 0.008 pb at [Formula: see text] GeV for the
             gluon-fusion production mode and from 0.31 pb at [Formula:
             see text] GeV to 0.009 pb at [Formula: see text] GeV for
             the vector-boson-fusion production mode. The results are
             also interpreted in the context of Type-I and Type-II
             two-Higgs-doublet models.},
   Doi = {10.1140/epjc/s10052-015-3820-z},
   Key = {fds321129}
}

@article{fds356701,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for an invisibly decaying Higgs boson or dark matter
             candidates produced in association with a Z boson in pp
             collisions at s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {776},
   Pages = {318-337},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2017.11.049},
   Abstract = {A search for an invisibly decaying Higgs boson or dark
             matter candidates produced in association with a
             leptonically decaying Z boson in proton–proton collisions
             at s=13 TeV is presented. This search uses 36.1 fb−1 of
             data collected by the ATLAS experiment at the Large Hadron
             Collider. No significant deviation from the expectation of
             the Standard Model backgrounds is observed. Assuming the
             Standard Model ZH production cross-section, an observed
             (expected) upper limit of 67% (39%) at the 95% confidence
             level is set on the branching ratio of invisible decays of
             the Higgs boson with mass mH=125 GeV. The corresponding
             limits on the production cross-section of the ZH process
             with the invisible Higgs boson decays are also presented.
             Furthermore, exclusion limits on the dark matter candidate
             and mediator masses are reported in the framework of
             simplified dark matter models.},
   Doi = {10.1016/j.physletb.2017.11.049},
   Key = {fds356701}
}

@article{fds356762,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Search for anomalous electroweak production of WW /WZ in
             association with a high-mass dijet system in pp collisions
             at s =8 TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {95},
   Number = {3},
   Year = {2017},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.95.032001},
   Abstract = {A search is presented for anomalous quartic gauge boson
             couplings in vector-boson scattering. The data for the
             analysis correspond to 20.2 fb-1 of s=8 TeV pp collisions
             and were collected in 1972 by the ATLAS experiment at the
             Large Hadron Collider. The search looks for the production
             of WW or WZ boson pairs accompanied by a high-mass dijet
             system, with one W decaying leptonically and a W or Z
             decaying hadronically. The hadronically decaying W/Z is
             reconstructed as either two small-radius jets or one
             large-radius jet using jet substructure techniques.
             Constraints on the anomalous quartic gauge boson coupling
             parameters α4 and α5 are set by fitting the transverse
             mass of the diboson system, and the resulting 95% confidence
             intervals are -0.024<α4<0.030 and -0.028<α5<0.033.},
   Doi = {10.1103/PhysRevD.95.032001},
   Key = {fds356762}
}

@article{fds352492,
   Author = {Acosta, and D, and others},
   Title = {Search for anomalous kinematics in t anti-t dilepton events
             at CDF II},
   Journal = {Phys. Rev. Lett.},
   Volume = {95},
   Number = {2},
   Pages = {022001},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/physrevlett.95.022001},
   Abstract = {http://arxiv.org/abs/hep-ex/0412042},
   Doi = {10.1103/physrevlett.95.022001},
   Key = {fds352492}
}

@article{fds308149,
   Author = {Acosta, and D, and others},
   Title = {Search for anomalous production of diphoton events with
             missing transverse energy at CDF and limits on gauge-
             mediated supersymmetry-breaking models},
   Journal = {Phys. Rev.},
   Volume = {D71},
   Number = {3},
   Pages = {031104},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.031104},
   Abstract = {http://arxiv.org/abs/hep-ex/0410053},
   Doi = {10.1103/PhysRevD.71.031104},
   Key = {fds308149}
}

@article{fds307978,
   Author = {Aaltonen, T and others},
   Title = {Search for anomalous production of events with a photon,
             jet, b-quark jet, and missing transverse
             energy},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {5},
   Pages = {052003},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.052003},
   Abstract = {We present a signature-based search for the anomalous
             production of events containing a photon, two jets, of which
             at least one is identified as originating from a b quark,
             and missing transverse energy (E̸T). The search uses data
             corresponding to 2.0  fb-1 of integrated luminosity from
             pp̅ collisions at a center-of-mass energy of
             sqrt[s]=1.96  TeV, collected with the CDF II detector at
             the Fermilab Tevatron. From 6.697 47×106 events with a
             photon candidate with transverse energy ET&gt;25  GeV,
             we find 617 events with E̸T&gt;25  GeV and two or more
             jets with ET&gt;15  GeV, at least one identified as
             originating from a b quark, versus an expectation of 607
             &plusmn; 113 events. Increasing the requirement on E̸T to
             50 GeV, we find 28 events versus an expectation of 30
             &plusmn; 11 events. We find no indications of
             non-standard-model phenomena.},
   Doi = {10.1103/PhysRevD.80.052003},
   Key = {fds307978}
}

@article{fds307927,
   Author = {Aaltonen, and T, and others},
   Title = {Search for anomalous production of events with two photons
             and additional energetic objects at CDF},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {5},
   Pages = {052005},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.052005},
   Abstract = {We present results of a search for anomalous production of
             two photons together with an electron, muon, τ lepton,
             missing transverse energy, or jets using pp̄ collision data
             from 1.1-2.0fb-1 of integrated luminosity collected by the
             Collider Detector at Fermilab (CDF). The event yields and
             kinematic distributions are examined for signs of new
             physics without favoring a specific model of new physics.
             The results are consistent with the standard model
             expectations. The search employs several new analysis
             techniques that significantly reduce instrumental
             backgrounds in channels with an electron and missing
             transverse energy. © 2010 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.82.052005},
   Key = {fds307927}
}

@article{fds308059,
   Author = {Abulencia, and A, and others},
   Title = {Search for anomalous production of multi-lepton events in $p
             \bar{p}$ collisions at $\sqrt{s}$ = 1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {13},
   Pages = {131804},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.131804},
   Abstract = {We report a search for the anomalous production of events
             with multiple charged leptons in p[overline p] collisions at
             sqrt(s)=1.96 TeV using a data sample corresponding to an
             integrated luminosity of 346 pb-1 collected by the CDF II
             detector at the Fermilab Tevatron. The search is divided
             into three-lepton and four-or-more-lepton data samples. We
             observe six events in the three-lepton sample and zero
             events in the >=4-lepton sample. Both numbers of events are
             consistent with standard model background expectations.
             Within the framework of an R-parity-violating supergravity
             model, the results are interpreted as mass limits on the
             lightest neutralino (chi-tilde10) and chargino
             (chi-tilde1[plus-minus]) particles. For one particular
             choice of model parameters, the limits are
             M(chi-tilde10)>110 GeV/c2 and M(chi-tilde1[plus-minus])>203
             GeV/c2 at 95\% confidence level; the variation of these mass
             limits with model parameters is presented.},
   Doi = {10.1103/physrevlett.98.131804},
   Key = {fds308059}
}

@article{fds307818,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'errico, M},
   Title = {Search for anomalous production of multiple leptons in
             association with W and Z bosons at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.092001},
   Abstract = {This paper presents a search for anomalous production of
             multiple low-energy leptons in association with a W or Z
             boson using events collected at the CDF experiment
             corresponding to 5.1fb -1 of integrated luminosity. This
             search is sensitive to a wide range of topologies with
             low-momentum leptons, including those with the leptons near
             one another. The observed rates of production of additional
             electrons and muons are compared with the standard model
             predictions. No indications of phenomena beyond the standard
             model are found. A 95% confidence level limit is presented
             on the production cross section for a benchmark model of
             supersymmetric hidden-valley Higgs production. Particle
             identification efficiencies are also provided to enable the
             calculation of limits on additional models. © 2012 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.85.092001},
   Key = {fds307818}
}

@article{fds307659,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim, A and Amram,
             N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M},
   Title = {Search for anomalous production of prompt like-sign lepton
             pairs at √s =7 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {12},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP12(2012)007},
   Abstract = {An inclusive search for anomalous production of two prompt,
             isolated leptons with the same electric charge is presented.
             The search is performed in a data sample corresponding to
             4.7 fb-1 of integrated luminosity collected in 2011 at √s
             =7 TeV with the ATLAS detector at the LHC. Pairs of leptons
             (e± e±, e± μ ±, and μ ± μ ±) with large transverse
             momentum are selected, and the dilepton invariant mass
             distribution is examined for any deviation from the Standard
             Model expectation. No excess is found, and upper limits on
             the production cross section of like-sign lepton pairs from
             physics processes beyond the Standard Model are placed as a
             function of the dilepton invariant mass within a fiducial
             region close to the experimental selection criteria. The 95%
             confidence level upper limits on the cross section of
             anomalous e± e ±, e± μ ±, or μ ± μ ± production
             range between 1.7 fb and 64 fb depending on the dilepton
             mass and flavour combination. © 2012 Cern for the benefit
             of the ATLAS collaboration.},
   Doi = {10.1007/JHEP12(2012)007},
   Key = {fds307659}
}

@article{fds307738,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for anomalous production of prompt like-sign muon
             pairs and constraints on physics beyond the standard model
             with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.032004},
   Abstract = {An inclusive search for anomalous production of two prompt,
             isolated muons with the same electric charge is presented.
             The search is performed in a data sample corresponding to
             1.6fb-1 of integrated luminosity collected in 2011 at
             √s=7TeV with the ATLAS detector at the LHC. Muon pairs are
             selected by requiring two isolated muons of the same
             electric charge with p T>20GeV and |η|<2.5. Minimal
             requirements are placed on the rest of the event activity.
             The distribution of the invariant mass of the muon pair
             m(μμ) is found to agree well with the background
             expectation. Upper limits on the cross section for anomalous
             production of two muons with the same electric charge are
             placed as a function of m(μμ) within a fiducial region
             defined by the event selection. The fiducial cross-section
             limit constrains the like-sign top-quark pair-production
             cross section to be below 3.7pb at 95% confidence level. The
             data are also analyzed to search for a narrow like-sign
             dimuon resonance as predicted for e.g. doubly charged Higgs
             bosons (H ±). Assuming pair production of H± bosons and a
             branching ratio to muons of 100% (33%), this analysis
             excludes masses below 355 (244)GeV and 251 (209)GeV for H±
             bosons coupling to left-handed and right-handed fermions,
             respectively. © 2012 CERN. Published by the American
             Physical Society under the terms of the uri
             xlink:href=http://creativecommons.org/licenses/by/3.0/Creative
             Commons Attribution 3.0 License. Further distribution of
             this work must maintain attribution to the author(s) and the
             published article's title, journal citation, and DOI. ©
             2012 American Physical Society.},
   Doi = {10.1103/PhysRevD.85.032004},
   Key = {fds307738}
}

@article{fds310295,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for anomalous production of prompt same-sign lepton
             pairs and pair-produced doubly charged Higgs bosons with s
             =8 TeV pp collisions using the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP03(2015)041},
   Abstract = {Abstract: A low-background inclusive search for new physics
             in events with same-sign dileptons is presented. The search
             uses proton-proton collisions corresponding to 20.3 fb−1
             of integrated luminosity taken in 2012 at a centre-of-mass
             energy of 8 TeV with the ATLAS detector at the LHC. Pairs of
             isolated leptons with the same electric charge and large
             transverse momenta of the type e±e±, e±μ±, and μ±μ±
             are selected and their invariant mass distribution is
             examined. No excess of events above the expected level of
             Standard Model background is found. The results are used to
             set upper limits on the cross-sections for processes beyond
             the Standard Model. Limits are placed as a function of the
             dilepton invariant mass within a fiducial region
             corresponding to the signal event selection criteria.
             Exclusion limits are also derived for a specific model of
             doubly charged Higgs boson production.[Figure not available:
             see fulltext.]},
   Doi = {10.1007/JHEP03(2015)041},
   Key = {fds310295}
}

@article{fds308114,
   Author = {Abulencia, and A, and others},
   Title = {Search for anomalous semileptonic decay of heavy flavor
             hadrons produced in association with a W boson at CDF
             II},
   Journal = {Phys. Rev.},
   Volume = {D73},
   Number = {5},
   Pages = {051101},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.051101},
   Abstract = {We present a search for anomalous semileptonic decays of
             heavy flavor hadrons produced in association with a W boson,
             in proton-antiproton collisions at s**(1/2) = 1.96 TeV. We
             use 162 pb-1 of data collected with the CDF II detector at
             the Fermilab Tevatron Collider. We select events with one W
             boson and at least one jet with an identified secondary
             vertex. In the jets with a secondary vertex we look for a
             semileptonic decay to a muon. We compare the number of jets
             with both a secondary vertex and a semileptonic decay, and
             the kinematic properties of these jets, with the standard
             model expectation, and we set limits on the production cross
             section of a B-like hadron with an anomalously high
             semileptonic branching ratio.},
   Doi = {10.1103/PhysRevD.73.051101},
   Key = {fds308114}
}

@article{fds307825,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A},
   Title = {Search for anomaly-mediated supersymmetry breaking with the
             ATLAS detector based on a disappearing-track signature in pp
             collisions at √s=7 TeV},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {4},
   Pages = {1-20},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-1993-2},
   Abstract = {In models of anomaly-mediated supersymmetry breaking (AMSB),
             the lightest chargino is predicted to have a lifetime long
             enough to be detected in collider experiments. This letter
             explores AMSB scenarios in pp collisions at (Formula
             Presented) = 7 TeV by attempting to identify decaying
             charginos which result in tracks that appear to have few
             associated hits in the outer region of the tracking system.
             The search was based on data corresponding to an integrated
             luminosity of 1.02 fb−1collected with the ATLAS detector
             in 2011. The pT spectrum of candidate tracks is found to be
             consistent with the expectation from Standard Model
             background processes and constraints on the lifetime and the
             production cross section were obtained. In the minimal AMSB
             framework with m3/2< 32 TeV, m0< 1.5 TeV, tanβ = 5 and μ >
             0, a chargino having mass below 92 GeV and a lifetime
             between 0.5 ns and 2 ns is excluded at 95 % confidence
             level.},
   Doi = {10.1140/epjc/s10052-012-1993-2},
   Key = {fds307825}
}

@article{fds356699,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for B - L R-parity-violating top squarks in √s=13
             TeV pp collisions with the ATLAS experiment},
   Journal = {Physical Review D},
   Volume = {97},
   Number = {3},
   Year = {2018},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.97.032003},
   Abstract = {A search is presented for the direct pair production of the
             stop, the supersymmetric partner of the top quark, that
             decays through an R-parity-violating coupling to a final
             state with two leptons and two jets, at least one of which
             is identified as a b-jet. The data set corresponds to an
             integrated luminosity of 36.1 fb-1 of proton-proton
             collisions at a center-of-mass energy of √s= 13 TeV,
             collected in 2015 and 2016 by the ATLAS detector at the LHC.
             No significant excess is observed over the Standard Model
             background, and exclusion limits are set on stop pair
             production at a 95% confidence level. Lower limits on the
             stop mass are set between 600 GeV and 1.5 TeV for branching
             ratios above 10% for decays to an electron or muon and a
             b-quark.},
   Doi = {10.1103/PhysRevD.97.032003},
   Key = {fds356699}
}

@article{fds308165,
   Author = {Acousta, D and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, J-F and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
             J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura, P and Campanelli, M and Campbell, M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, W-H and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat,
             C and Cyr, D and Dagenhart, D and Da Ronco and S and D'Auria, S and de
             Barbaro, P and De Cecco and S and De Lentdecker and G and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Dininno, M and De Pedis,
             D and Derwent, PF and Devlin, T and Dionisi, C and Dittmann, JR and Doksus,
             P and Dominguez, A and Donati, S and Donega, M and D'Onnofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, H-C and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan,
             G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester,
             S and Foster, GW and Franklin, M and Frisch, H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Gondcharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra,
             Y and Goulianos, K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Guimaraes da Costa and J and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans,
             D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Karagoz Unel and M and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Kongisberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
             SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin,
             CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lukens, P and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martiínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Moulik, T and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, A-S and Nigmanov, T and Nodulman, L and Oesterberg, K and Ogawa, T and Oh, S and Oh, YD and Ohsugi, T and Okusawa,
             T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pitts, KT and Plager, C and Pompos, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio,
             S and Ratnikov, F and Ray, H and Reichold, A and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson,
             WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and St Denis and R and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Sfiligoi, I and Shears,
             T and Scribano, A and Scuri, F and Sefov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Shapiro, MD and Shepard, PF and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba, A and Slaughter, AJ and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Somalwar, SV and Spalding, J and Spezziga, M and Spiegel, L and Spinella, F and Spiropulu, M and Squillacioti, P and Stadie,
             H},
   Title = {Search for B0s-->micro+micro- and B0d-->micro+micro- decays
             in pp collisions at square root s = 1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {93},
   Number = {3},
   Pages = {032001},
   Year = {2004},
   Month = {July},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.93.032001},
   Abstract = {We report on a search for B(0)(s)-->micro(+)micro(-) and
             B(0)(d)-->micro(+)micro(-) decays in pp collisions at square
             root of s=1.96 TeV using 171 pb(-1) of data collected by the
             CDF II experiment at the Fermilab Tevatron Collider. The
             decay rates of these rare processes are sensitive to
             contributions from physics beyond the standard model. One
             event survives all our selection requirements, consistent
             with the background expectation. We derive branching ratio
             limits of B(B(0)(s)-->micro(+)micro(-))<5.8x10(-7) and
             B(B(0)(d)-->micro(+)micro(-))<1.5x10(-7) at 90% confidence
             level.},
   Doi = {10.1103/physrevlett.93.032001},
   Key = {fds308165}
}

@article{fds308154,
   Author = {al, DAE},
   Title = {Search for B0s-->µ+µ- and B0d-->µ+µ- Decays in pp-bar
             Collisions at sqrt[s]=1.96 TeV},
   Journal = {Physical Review Letters},
   Volume = {93},
   Number = {5},
   Pages = {032001},
   Publisher = {American Physical Society (APS)},
   Year = {2004},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.72.051104},
   Abstract = {We report on a search for B0s-->µ+µ- and B0d-->µ+µ-
             decays in pp-bar collisions at sqrt[s]=1.96 TeV using 171
             pb-1 of data collected by the CDF II experiment at the
             Fermilab Tevatron Collider. The decay rates of these rare
             processes are sensitive to contributions from physics beyond
             the standard model. One event survives all our selection
             requirements, consistent with the background expectation. We
             derive branching ratio limits of B(B0s--
             >µ+µ-)µ+µ-)},
   Doi = {10.1103/PhysRevD.72.051104},
   Key = {fds308154}
}

@article{fds321085,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel,
             C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
             Navarro, L and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
             A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El
             Moursli, RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M},
   Title = {Search for bottom squark pair production in proton-proton
             collisions at [Formula: see text] TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {10},
   Pages = {547},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4382-4},
   Abstract = {The result of a search for pair production of the
             supersymmetric partner of the Standard Model bottom quark
             ([Formula: see text]) is reported. The search uses
             3.2 fb[Formula: see text]  of <i>pp</i> collisions at
             [Formula: see text] TeV collected by the ATLAS experiment
             at the Large Hadron Collider in 2015. Bottom squarks are
             searched for in events containing large missing transverse
             momentum and exactly two jets identified as originating from
             <i>b</i>-quarks. No excess above the expected Standard Model
             background yield is observed. Exclusion limits at 95 %
             confidence level on the mass of the bottom squark are
             derived in phenomenological supersymmetric
             <i>R</i>-parity-conserving models in which the [Formula: see
             text] is the lightest squark and is assumed to decay
             exclusively via [Formula: see text], where [Formula: see
             text] is the lightest neutralino. The limits significantly
             extend previous results; bottom squark masses up to 800
             (840) GeV are excluded for the [Formula: see text] mass
             below 360 (100) GeV whilst differences in mass above
             100 GeV between the [Formula: see text] and the [Formula:
             see text] are excluded up to a [Formula: see text] mass of
             500 GeV.},
   Doi = {10.1140/epjc/s10052-016-4382-4},
   Key = {fds321085}
}

@article{fds308220,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon,
             R and Briskin, G and Brock, R and Bross, A and Buchholz, D and Burtovoi,
             VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
             M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Signore,
             KD and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Loreto, GD and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum,
             E},
   Title = {Search for bottom squarks in [formula presented] collisions
             at [formula presented]},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {60},
   Number = {3},
   Pages = {1-5},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.60.031101},
   Abstract = {We report on a search for bottom squarks (Formula presented)
             produced in (Formula presented) collisions at (Formula
             presented) using the DØ detector at Fermilab. Bottom
             squarks are assumed to be produced in pairs and to decay to
             the lightest supersymmetric particle (LSP) and a b quark
             with a branching fraction of 100%. The LSP is assumed to be
             the lightest neutralino and stable. We set limits on the
             production cross section as a function of (Formula
             presented) mass and LSP mass. © 1999 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.60.031101},
   Key = {fds308220}
}

@article{fds356557,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
             V},
   Title = {Search for bottom-squark pair production with the ATLAS
             detector in final states containing Higgs bosons, b-jets and
             missing transverse momentum},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {12},
   Year = {2019},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2019)060},
   Abstract = {The result of a search for the pair production of the
             lightest supersymmetric partner of the bottom quark (b˜ 1)
             using 139 fb−1 of proton-proton data collected at s = 13
             TeV by the ATLAS detector is reported. In the supersymmetric
             scenarios considered both of the bottom-squarks decay into a
             b-quark and the second-lightest neutralino, b˜1→b+χ˜20.
             Each χ˜20 is assumed to subsequently decay with 100%
             branching ratio into a Higgs boson (h) like the one in the
             Standard Model and the lightest neutralino:
             χ˜20→h+χ˜10. The χ˜10 is assumed to be the lightest
             supersymmetric particle (LSP) and is stable. Two signal mass
             configurations are targeted: the first has a constant LSP
             mass of 60 GeV; and the second has a constant mass
             difference between the χ˜20 and χ˜10 of 130 GeV. The
             final states considered contain no charged leptons, three or
             more b-jets, and large missing transverse momentum. No
             significant excess of events over the Standard Model
             background expectation is observed in any of the signal
             regions considered. Limits at the 95% confidence level are
             placed in the supersymmetric models considered, and
             bottom-squarks with mass up to 1.5 TeV are excluded. [Figure
             not available: see fulltext.]},
   Doi = {10.1007/JHEP12(2019)060},
   Key = {fds356557}
}

@article{fds308036,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
             T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
             F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and De
             Lorenzo, G and Dell'orso, M and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di
             Ruzza, B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
             C and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt,
             J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
             S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson,
             W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Koay, SA and Kondo,
             K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus,
             J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
             C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli, F and Marino, C and Marino, CP and Martin,
             A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín,
             R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
             A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello,
             M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
             A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna,
             G and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria,
             A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J},
   Title = {Search for Bs0 --> micro+ micro- and B0 --> micro+ micro-
             decays with 2 fb-1 of pp collisions.},
   Journal = {Physical review letters},
   Volume = {100},
   Number = {10},
   Pages = {101802},
   Year = {2008},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.100.101802},
   Abstract = {We have performed a search for B(s)(0) --> micro(+) micro(-)
             and B(0) --> micro(+) micro(-) decays in pp collisions at
             square root s = 1.96 TeV using 2 fb(-1) of integrated
             luminosity collected by the CDF II detector at the Fermilab
             Tevatron Collider. The observed number of B(s)(0) and B0
             candidates is consistent with background expectations. The
             resulting upper limits on the branching fractions are
             B(B(s)0) --> micro(+) micro(-)) <5.8 x 10(-8) and B(B(0) -->
             micro(+) micro(-))<1.8 x 10(-8) at 95% C.L.},
   Doi = {10.1103/physrevlett.100.101802},
   Key = {fds308036}
}

@article{fds313579,
   Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'orso, M and Deluca,
             C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'errico,
             M and Canto, AD and Ruzza, BD and Dittmann, JR and D'onofrio, M and Donati,
             S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
             JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
             MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
             MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
             E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and Mcfarland, KS and Mcintyre, P and Mcnulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Sperka, D and Squillacioti, P and Stancari, M and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang, YC},
   Title = {Search for Bs0→μ+μ- and
             B0→μ+μ- decays with CDF
             II},
   Journal = {Physical Review Letters},
   Volume = {107},
   Number = {19},
   Pages = {191801},
   Year = {2011},
   url = {http://www.ncbi.nlm.nih.gov/pubmed/22181596},
   Abstract = {A search has been performed for Bs0→μ+μ- and B0→μ+μ-
             decays using 7fb-1 of integrated luminosity collected by the
             CDF II detector at the Fermilab Tevatron collider. The
             observed number of B0 candidates is consistent with
             background-only expectations and yields an upper limit on
             the branching fraction of B(B0→μ+μ-)&lt;6.0×10-9 at 95%
             confidence level. We observe an excess of Bs0 candidates.
             The probability that the background processes alone could
             produce such an excess or larger is 0.27%. The probability
             that the combination of background and the expected standard
             model rate of Bs0→μ+μ- could produce such an excess or
             larger is 1.9%. These data are used to determine
             B(Bs0→μ+μ-)=(1.8-0.9+1.1)×10 -8 and provide an upper
             limit of B(Bs0→μ+μ -)&lt;4.0×10-8 at 95% confidence
             level. © 2011 American Physical Society.},
   Doi = {10.1103/PhysRevLett.107.191801},
   Key = {fds313579}
}

@article{fds307607,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Search for Bs0→μ+μ- and
             B0→μ+μ- decays with the full CDF
             Run II data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.072003},
   Abstract = {We report on a search for Bs0→μ+μ- and B0→μ+μ-
             decays using proton-antiproton collision data at √s=1.96
             TeV corresponding to 10 fb-1 of integrated luminosity
             collected by the CDF II detector at the Fermilab Tevatron
             collider. The observed number of B0 candidates is consistent
             with background-only expectations and yields an upper limit
             on the branching fraction of B(B0→μ+μ-)<4.6×10-9 at 95%
             confidence level. We observe an excess of Bs0 candidates.
             The probability that the background processes alone could
             produce such an excess or larger is 0.94%. The probability
             that the combination of background and the expected standard
             model rate of Bs0→μ+μ- could produce such an excess or
             larger is 6.8%. These data are used to determine a branching
             fraction B(Bs0→μ+μ-)=(1.3-0.7+0.9) ×10-8 and provide an
             upper limit of B(Bs0→μ +μ-)<3.1×10-8 at 95% confidence
             level. © 2013 American Physical Society.},
   Doi = {10.1103/PhysRevD.87.072003},
   Key = {fds307607}
}

@booklet{Abbott98g,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
             EW and Goussiou, A and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Dugad, SR and Bantly,
             J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram,
             I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Astur, R and Biswas,
             N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko,
             NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross,
             A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Valdez, CH and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger,
             C and Vidal, CD and Cummings, MA and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
             SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
             Y and Dudko, LV and Banerjee, S and Edmunds, D and Ellison, J and Elvira,
             VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
             OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein,
             D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum,
             E and Forden, GE},
   Title = {Search for charge-1/3 Third-generation leptoquarks in p¯p
             collisions at √s=1.8TeV},
   Journal = {Physical Review Letters},
   Volume = {81},
   Number = {1},
   Pages = {38-43},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.81.38},
   Abstract = {We report on a search for charge-1/3 third-generation
             leptoquarks (LQ) produced in p¯p collisions at √s=1.8TeV
             using the D0 detector at Fermilab. Third-generation
             leptoquarks are assumed to be produced in pairs and to decay
             to a tau neutrino and a b quark with branching fraction B.
             We place upper limits on σ (p¯p→LQ¯LQ)B2 as a function
             of the leptoquark mass MLQ. Assuming B=1 we exclude at the
             95% confidence level third-generation scalar leptoquarks
             with MLQ<94GeV/c2 and third-generation vector leptoquarks
             with MLQ<216GeV/c2(MLQ<148GeV/c2) assuming Yang-Mills
             (anomalous) coupling. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.81.38},
   Key = {Abbott98g}
}

@article{fds357501,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
             C},
   Title = {Search for charged Higgs bosons decaying into a top quark
             and a bottom quark at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {6},
   Year = {2021},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2021)145},
   Abstract = {A search for charged Higgs bosons decaying into a top quark
             and a bottom quark is presented. The data analysed
             correspond to 139 fb−1 of proton-proton collisions at s =
             13 TeV, recorded with the ATLAS detector at the LHC. The
             production of a heavy charged Higgs boson in association
             with a top quark and a bottom quark, pp → tbH+ → tbtb,
             is explored in the H+ mass range from 200 to 2000 GeV using
             final states with jets and one electron or muon. Events are
             categorised according to the multiplicity of jets and
             b-tagged jets, and multivariate analysis techniques are used
             to discriminate between signal and background events. No
             significant excess above the background-only hypothesis is
             observed and exclusion limits are derived for the production
             cross-section times branching ratio of a charged Higgs boson
             as a function of its mass; they range from 3.6 pb at 200 GeV
             to 0.036 pb at 2000 GeV at 95% confidence level. The results
             are interpreted in the hMSSM and Mh125 scenarios. [Figure
             not available: see fulltext.]},
   Doi = {10.1007/JHEP06(2021)145},
   Key = {fds357501}
}

@article{fds356646,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Search for charged Higgs bosons decaying into top and bottom
             quarks at √s=13 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {11},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2018)085},
   Abstract = {A search for charged Higgs bosons heavier than the top quark
             and decaying via H± → tb is presented. The data analysed
             corresponds to 36.1 fb−1 of pp collisions at s=13 TeV and
             was recorded with the ATLAS detector at the LHC in 2015 and
             2016. The production of a charged Higgs boson in association
             with a top quark and a bottom quark, pp → tbH±, is
             explored in the mass range from mH± = 200 to 2000 GeV using
             multi-jet final states with one or two electrons or muons.
             Events are categorised according to the multiplicity of jets
             and how likely these are to have originated from
             hadronisation of a bottom quark. Multivariate techniques are
             used to discriminate between signal and background events.
             No significant excess above the background-only hypothesis
             is observed and exclusion limits are derived for the
             production cross-section times branching ratio of a charged
             Higgs boson as a function of its mass, which range from 2.9
             pb at mH± = 200 GeV to 0.070 pb at mH± = 2000 GeV. The
             results are interpreted in two benchmark scenarios of the
             Minimal Supersymmetric Standard Model.[Figure not available:
             see fulltext.].},
   Doi = {10.1007/JHEP11(2018)085},
   Key = {fds356646}
}

@article{fds356665,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Search for charged Higgs bosons decaying via H ±
             → τ ± ντ in the τ+jets and
             τ+lepton final states with 36 fb−1 of pp
             collision data recorded at √s=13 TeV with the ATLAS
             experiment},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {9},
   Year = {2018},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2018)139},
   Abstract = {Charged Higgs bosons produced either in top-quark decays or
             in association with a top-quark, subsequently decaying via
             H± → τ±ντ, are searched for in 36.1 fb−1 of
             proton-proton collision data at s=13 TeV recorded with the
             ATLAS detector. Depending on whether the top-quark produced
             together with H± decays hadronically or leptonically, the
             search targets τ+jets and τ+lepton final states, in both
             cases with a hadronically decaying τ-lepton. No evidence of
             a charged Higgs boson is found. For the mass range of mH± =
             90–2000 GeV, upper limits at the 95% confidence level are
             set on the production cross-section of the charged Higgs
             boson times the branching fraction ℬ (H±→ τ±ντ) in
             the range 4.2–0.0025 pb. In the mass range 90–160 GeV,
             assuming the Standard Model cross-section for tt¯
             production, this corresponds to upper limits between 0.25%
             and 0.031% for the branching fraction ℬ(t→bH±)×ℬ(H±→τ±ντ).[Figure
             not available: see fulltext.]},
   Doi = {10.1007/JHEP09(2018)139},
   Key = {fds356665}
}

@article{fds313592,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos,
             S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold,
             H},
   Title = {Search for charged Higgs bosons decaying via H±
             → τ±ν in fully hadronic final states using
             pp collision data at √s = 8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2015)088},
   Abstract = {Abstract: The results of a search for charged Higgs bosons
             decaying to a τ lepton and a neutrino, H± → τ±ν, are
             presented. The analysis is based on 19.5 fb−1 of
             proton-proton collision data at s$$ \sqrt{s} $$ = 8 TeV
             collected by the ATLAS experiment at the Large Hadron
             Collider. Charged Higgs bosons are searched for in events
             consistent with top-quark pair production or in associated
             production with a top quark, depending on the considered H±
             mass. The final state is characterised by the presence of a
             hadronic τ decay, missing transverse momentum, b-tagged
             jets, a hadronically decaying W boson, and the absence of
             any isolated electrons or muons with high transverse
             momenta. The data are consistent with the expected
             background from Standard Model processes. A statistical
             analysis leads to 95% confidence-level upper limits on the
             product of branching ratios ℬ(t → bH±) × ℬ(H± →
             τ±ν), between 0.23% and 1.3% for charged Higgs boson
             masses in the range 80-160GeV. It also leads to 95%
             confidence-level upper limits on the production cross
             section times branching ratio, σ(pp → tH± + X) ×
             ℬ(H± → τ±ν), between 0.76 pb and 4.5 fb, for
             charged Higgs boson masses ranging from 180 GeV to 1000 GeV.
             In the context of different scenarios of the Minimal
             Supersymmetric Standard Model, these results exclude nearly
             all values of tan β above one for charged Higgs boson
             masses between 80 GeV and 160 GeV, and exclude a region of
             parameter space with high tan β for H± masses between 200
             GeV and 250 GeV.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP03(2015)088},
   Key = {fds313592}
}

@article{fds307789,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwoo-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio, LB and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {Search for charged Higgs bosons decaying via H±
             → τν in tt̄ events using pp collision data at √s = 7
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP06(2012)039},
   Abstract = {The results of a search for charged Higgs bosons are
             presented. The analysis is based on 4.6 fb?1 of
             proton-proton collision data at √s = 7TeV collected by the
             ATLAS experiment at the Large Hadron Collider, using top
             quark pair events with a τ lepton in the final state. The
             data are consistent with the expected background from
             Standard Model processes. Assuming that the branching ratio
             of the charged Higgs boson to a τ lepton and a neutrino is
             100%, this leads to upper limits on the branching ratio of
             top quark decays to a b quark and a charged Higgs boson
             between 5% and 1% for charged Higgs boson masses ranging
             from 90GeV to 160GeV, respectively. In the context of the
             mhmaxscenario of the MSSM, tan β above 12-26, as well as
             between 1 and 2-6, can be excluded for charged Higgs boson
             masses between 90GeV and 150GeV. Copyright
             CERN.},
   Doi = {10.1007/JHEP06(2012)039},
   Key = {fds307789}
}

@article{fds308103,
   Author = {Abulencia, and A, and others},
   Title = {Search for charged Higgs bosons from top quark decays in p
             anti-p collisions at $\sqrt{s}$ = 1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {4},
   Pages = {042003},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.042003},
   Abstract = {We report the results of a search for a charged Higgs boson
             in the decays of top quarks produced in p anti-p collisions
             at a center-of-mass energy of 1.96 GeV. We use a data sample
             corresponding to an integrated luminosity of 193 pb-1
             collected by the upgraded Collider Detector at Fermilab. No
             evidence for charged Higgs production is found, allowing 95%
             C.L. upper limits to be placed on BR(t --> H+b) for
             different charged Higgs decay scenarios. In addition, we
             present in the MSSM (m_H+/-, tan B) plane the first
             exclusion regions with radiative and Yukawa coupling
             corrections.},
   Doi = {10.1103/physrevlett.96.042003},
   Key = {fds308103}
}

@article{fds308224,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Alves, GA and Amos, N and Anderson,
             EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov,
             VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland,
             T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {Search for charged higgs bosons in decays of top quark
             pairs},
   Journal = {Physical Review Letters},
   Volume = {82},
   Number = {25},
   Pages = {4975-4980},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.82.4975},
   Abstract = {We present a search for charged Higgs bosons in decays of
             pair-produced top quarks using 109.2 ± 5.8pb-1 of data
             recorded from pp collisions at √ s = 1.8 TeV by the D0
             detector during 1992-1996 at the Fermilab Tevatron. No
             evidence is found for charged Higgs production, and most
             parts of the [MH+, tan β] parameter space where the decay t
             → H+ b has a branching fraction close to or larger than
             that for t → W+ b are excluded at 95% confidence level.
             Assuming mt = 175 GeV and σ(pp → tt) = 5.5 pb, for MH+ =
             60 GeV, we exclude tan β < 0.97 and tan β > 40.9. © 1999
             The American Physical Society.},
   Doi = {10.1103/PhysRevLett.82.4975},
   Key = {fds308224}
}

@article{fds307943,
   Author = {Aaltonen, T and others},
   Title = {Search for Charged Higgs Bosons in Decays of Top Quarks in
             pp̅ Collisions at sqrt[s] =1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {10},
   Pages = {101803},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.101803},
   Abstract = {We report on the first direct search for charged Higgs
             bosons decaying into cs̅ in tt̅ events produced by pp̅
             collisions at sqrt[s]=1.96  TeV. The search uses a data
             sample corresponding to an integrated luminosity of
             2.2  fb-1 collected by the CDF II detector at Fermilab
             and looks for a resonance in the invariant mass distribution
             of two jets in the lepton+jets sample of tt̅ candidates. We
             observe no evidence of charged Higgs bosons in top quark
             decays. Hence, 95% upper limits on the top quark decay
             branching ratio are placed at B(t→H+b)&lt; 0.1 to 0.3 for
             charged Higgs boson masses of 60 to 150  GeV/c2 assuming
             B(H+→cs̅ )=1.0. The upper limits on B(t→H+b) are also
             used as model-independent limits on the decay branching
             ratio of top quarks to generic scalar charged bosons beyond
             the standard model.},
   Doi = {10.1103/physrevlett.103.101803},
   Key = {fds307943}
}

@article{fds356773,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Search for charged Higgs bosons in the H± → tb
             decay channel in pp collisions at √s = 8 TeV using the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {3},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2016)127},
   Abstract = {Charged Higgs bosons heavier than the top quark and decaying
             via H± → tb are searched for in proton-proton collisions
             measured with the ATLAS experiment at (Formula presented.)
             TeV corresponding to an integrated luminosity of 20.3fb−1.
             The production of a charged Higgs boson in association with
             a top quark, gb → tH±, is explored in the mass range 200
             to 600 GeV using multi-jet final states with one electron or
             muon. In order to separate the signal from the Standard
             Model background, analysis techniques combining several
             kinematic variables are employed. An excess of events above
             the background-only hypothesis is observed across a wide
             mass range, amounting to up to 2.4 standard deviations.
             Upper limits are set on the gb → tH± production cross
             section times the branching fraction BR(H± → tb).
             Additionally, the complementary s-channel production, qq′
             → H±, is investigated through a reinterpretation of W′
             → tb searches in ATLAS. Final states with one electron or
             muon are relevant for H± masses from 0.4 to 2.0 TeV,
             whereas the all-hadronic final state covers the range 1.5 to
             3.0 TeV. In these search channels, no significant excesses
             from the predictions of the Standard Model are observed, and
             upper limits are placed on the qq′ → H± production
             cross section times the branching fraction BR(H± →
             tb).},
   Doi = {10.1007/JHEP03(2016)127},
   Key = {fds356773}
}

@article{fds321101,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for charged Higgs bosons produced in association with
             a top quark and decaying via H± → τν using
             pp collision data recorded at √s=13 TeV by the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {759},
   Pages = {555-574},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.06.017},
   Abstract = {Charged Higgs bosons produced in association with a single
             top quark and decaying via H±→τν are searched for with
             the ATLAS experiment at the LHC, using proton–proton
             collision data at s=13 TeV corresponding to an integrated
             luminosity of 3.2 fb−1. The final state is characterised
             by the presence of a hadronic τ decay and missing
             transverse momentum, as well as a hadronically decaying top
             quark, resulting in the absence of high-transverse-momentum
             electrons and muons. The data are found to be consistent
             with the expected background from Standard Model processes.
             A statistical analysis leads to 95% confidence-level upper
             limits on the production cross section times branching
             fraction, σ(pp→[b]tH±)×BR(H±→τν), between 1.9 pb
             and 15 fb, for charged Higgs boson masses ranging from 200
             to 2000 GeV. The exclusion limits for this search surpass
             those obtained with the proton–proton collision data
             recorded at s=8 TeV.},
   Doi = {10.1016/j.physletb.2016.06.017},
   Key = {fds321101}
}

@article{fds307617,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Joffe, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
             S and Arik, E and Arik, M},
   Title = {Search for charged Higgs bosons through the violation of
             lepton universality in tt events using pp collision data at
             √S=7 TeV with the ATLAS experiment},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP03(2013)076},
   Abstract = {In several extensions of the Standard Model, the top quark
             can decay into a bottom quark and a light charged Higgs
             boson H +, t → bH +, in addition to the Standard Model
             decay t → bW. Since W bosons decay to the three lepton
             generations equally, while H + maypredominantlydecayinto
             τν, charged Higgs bosons can be searched for using the
             violation of lepton universality in top quark decays. The
             analysis in this paper is based on 4.6 fb-1 of proton-proton
             collision data at √s=7 TeV collected by the ATLAS
             experiment at the Large Hadron Collider. Signatures
             containing leptons (e or μ) and/or a hadronically decaying
             τ (τ had) are used. Event yield ratios between e + τ had
             and e + μ, as well as between μ + τ had andμ + e, final
             states are measured in the data and compared to predictions
             from simulations. This ratio-based method reduces the impact
             of systematic uncertainties in the analysis. No significant
             deviation from the Standard Model predictions is observed.
             With the assumption that the branching fraction ℬ (H + →
             τν) is 100%, upper limits in the range 3.2%-4.4% can be
             placed on the branching fraction ℬ (t → bH +) for
             charged Higgs boson masses m H+ in the range 90-140 GeV.
             After combination with results from a search for charged
             Higgs bosons in t\overline{t} decays using the τ had + jets
             final state, upper limits on ℬ (t → bH +) can be set in
             the range 0.8%-3.4%, for m H+ in the range 90-160
             GeV.[Figure not available: see fulltext.] © 2013 Cern for
             the benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP03(2013)076},
   Key = {fds307617}
}

@article{fds357654,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Zeid, OSA and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
             M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz,
             VA and Pereira, RA and Arcangeletti, C},
   Title = {Search for charged-lepton-flavour violation in Z-boson
             decays with the ATLAS detector},
   Journal = {Nature Physics},
   Volume = {17},
   Number = {7},
   Pages = {819-825},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {July},
   url = {http://dx.doi.org/10.1038/s41567-021-01225-z},
   Abstract = {Leptons with essentially the same properties apart from
             their mass are grouped into three families (or flavours).
             The number of leptons of each flavour is conserved in
             interactions, but this is not imposed by fundamental
             principles. Since the formulation of the standard model of
             particle physics, the observation of flavour oscillations
             among neutrinos has shown that lepton flavour is not
             conserved in neutrino weak interactions. So far, there has
             been no experimental evidence that this also occurs in
             interactions between charged leptons. Such an observation
             would be a sign of undiscovered particles or a yet unknown
             type of interaction. Here the ATLAS experiment at the Large
             Hadron Collider at CERN reports a constraint on
             lepton-flavour-violating effects in weak interactions,
             searching for Z-boson decays into a τ lepton and another
             lepton of different flavour with opposite electric charge.
             The branching fractions for these decays are measured to be
             less than 8.1 × 10−6 (eτ) and 9.5 × 10−6 (μτ) at
             the 95% confidence level using 139 fb−1 of proton–proton
             collision data at a centre-of-mass energy of s=13TeV and
             20.3 fb−1 at s=8TeV. These results supersede the limits
             from the Large Electron–Positron Collider experiments
             conducted more than two decades ago.},
   Doi = {10.1038/s41567-021-01225-z},
   Key = {fds357654}
}

@article{fds356586,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
             JF},
   Title = {Search for chargino and neutralino production in final
             states with a Higgs boson and missing transverse momentum at
             s =13 TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {100},
   Number = {1},
   Year = {2019},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.100.012006},
   Abstract = {A search is conducted for the electroweak pair production of
             a chargino and a neutralino pp→χ1±χ20, where the
             chargino decays into the lightest neutralino and a W boson,
             χ1±→χ10W±, while the neutralino decays into the
             lightest neutralino and a Standard Model-like 125 GeV Higgs
             boson, χ20→χ10h. Fully hadronic, semileptonic, diphoton,
             and multilepton (electrons, muons) final states with missing
             transverse momentum are considered in this search. Higgs
             bosons in the final state are identified by either two jets
             originating from bottom quarks (h→bb), two photons
             (h→γγ), or leptons from the decay modes h→WW, h→ZZ
             or h→ττ. The analysis is based on 36.1 fb-1 of s=13 TeV
             proton-proton collision data recorded by the ATLAS detector
             at the Large Hadron Collider. Observations are consistent
             with the Standard Model expectations, and 95%
             confidence-level limits of up to 680 GeV in χ1±/χ20 mass
             are set in the context of a simplified supersymmetric
             model.},
   Doi = {10.1103/PhysRevD.100.012006},
   Key = {fds356586}
}

@article{fds308048,
   Author = {Aaltonen, T and others},
   Title = {Search for Chargino-Neutralino Production in $p\overline p$
             Collisions at $\sqrt{s}$=1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {19},
   Pages = {191806},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.99.191806},
   Abstract = {We present a search for associated production of the
             chargino and neutralino supersymmetric particles using up to
             1.1 fb-1 of integrated luminosity collected by the CDF II
             experiment at the Tevatron p[overline p] collider at
             sqrt(s)=1.96 TeV. We analyze events with a large transverse
             momentum imbalance and either three charged leptons or two
             charged leptons of the same electric charge. The numbers of
             observed events are consistent with standard model
             expectations. Upper limits on the production cross section
             are derived in different theoretical models.},
   Doi = {10.1103/physrevlett.99.191806},
   Key = {fds308048}
}

@article{fds356650,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A},
   Title = {Search for chargino-neutralino production using recursive
             jigsaw reconstruction in final states with two or three
             charged leptons in proton-proton collisions at s =13 TeV
             with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {9},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.092012},
   Abstract = {A search for electroweak production of supersymmetric
             particles is performed in two-lepton and three-lepton final
             states using recursive jigsaw reconstruction, a technique
             that assigns reconstructed objects to the most probable
             hemispheres of the decay trees, allowing one to construct
             tailored kinematic variables to separate the signal and
             background. The search uses data collected in 2015 and 2016
             by the ATLAS experiment in s=13 TeV proton-proton collisions
             at the CERN Large Hadron Collider corresponding to an
             integrated luminosity of 36.1 fb-1. Chargino-neutralino pair
             production, with decays via W/Z bosons, is studied in final
             states involving leptons and jets and missing transverse
             momentum for scenarios with large and intermediate mass
             splittings between the parent particle and lightest
             supersymmetric particle, as well as for the scenario where
             this mass splitting is close to the mass of the Z boson. The
             latter case is challenging since the vector bosons are
             produced with kinematic properties that are similar to those
             in Standard Model processes. Results are found to be
             compatible with the Standard Model expectations in the
             signal regions targeting large and intermediate mass
             splittings, and chargino-neutralino masses up to 600 GeV are
             excluded at 95% confidence level for a massless lightest
             supersymmetric particle. Excesses of data above the expected
             background are found in the signal regions targeting low
             mass splittings, and the largest local excess amounts to 3.0
             standard deviations.},
   Doi = {10.1103/PhysRevD.98.092012},
   Key = {fds356650}
}

@article{fds349789,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
             Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V},
   Title = {Search for chargino-neutralino production with mass
             splittings near the electroweak scale in three-lepton final
             states in s =13 TeV pp collisions with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {101},
   Number = {7},
   Year = {2020},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.101.072001},
   Abstract = {A search for supersymmetry through the pair production of
             electroweakinos with mass splittings near the electroweak
             scale and decaying via on-shell W and Z bosons is presented
             for a three-lepton final state. The analyzed proton-proton
             collision data taken at a center-of-mass energy of s=13 TeV
             were collected between 2015 and 2018 by the ATLAS experiment
             at the Large Hadron Collider, corresponding to an integrated
             luminosity of 139 fb-1. A search, emulating the recursive
             jigsaw reconstruction technique with easily reproducible
             laboratory-frame variables, is performed. The two excesses
             observed in the 2015-2016 data recursive jigsaw analysis in
             the low-mass three-lepton phase space are reproduced.
             Results with the full data set are in agreement with the
             Standard Model expectations. They are interpreted to set
             exclusion limits at the 95% confidence level on simplified
             models of chargino-neutralino pair production for masses up
             to 345 GeV.},
   Doi = {10.1103/PhysRevD.101.072001},
   Key = {fds349789}
}

@article{fds307556,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {Search for charginos nearly mass degenerate with the
             lightest neutralino based on a disappearing-track signature
             in pp collisions at √(s) = 8 TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {11},
   Pages = {112006-1-112006-23},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.112006},
   Abstract = {A search is presented for direct chargino production based
             on a disappearing-track signature using 20:3 fb-1 of
             proton-proton collisions at √s = 8 TeV collected with the
             ATLAS experiment at the LHC. In anomaly-mediated
             supersymmetry breaking (AMSB) models, the lightest chargino
             is nearly mass degenerate with the lightest neutralino and
             its lifetime is long enough to be detected in the tracking
             detectors by identifying decays that result in tracks with
             no associated hits in the outer region of the tracking
             system. Some models with supersymmetry also predict
             charginos with a significant lifetime. This analysis attains
             sensitivity for charginos with a lifetime between 0.1 and 10
             ns, and significantly surpasses the reach of the LEP
             experiments. No significant excess above the background
             expectation is observed for candidate tracks with large
             transverse momentum, and constraints on chargino properties
             are obtained. In the AMSB scenarios, a chargino mass below
             270 GeV is excluded at 95% confidence level.},
   Doi = {10.1103/PhysRevD.88.112006},
   Key = {fds307556}
}

@article{fds361169,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
             Bella, L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos,
             S},
   Title = {Search for chargino–neutralino pair production in final
             states with three leptons and missing transverse momentum in
             √s=13 TeV pp collisions with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {12},
   Year = {2021},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09749-7},
   Abstract = {A search for chargino–neutralino pair production in
             three-lepton final states with missing transverse momentum
             is presented. The study is based on a dataset of s=13 TeV
             pp collisions recorded with the ATLAS detector at the LHC,
             corresponding to an integrated luminosity of 139 fb - 1. No
             significant excess relative to the Standard Model
             predictions is found in data. The results are interpreted in
             simplified models of supersymmetry, and statistically
             combined with results from a previous ATLAS search for
             compressed spectra in two-lepton final states. Various
             scenarios for the production and decay of charginos (χ~1±)
             and neutralinos (χ~20) are considered. For pure higgsino
             χ~1±χ~20 pair-production scenarios, exclusion limits at
             95% confidence level are set on χ~20 masses up to 210 GeV.
             Limits are also set for pure wino χ~1±χ~20 pair
             production, on χ~20 masses up to 640 GeV for decays via
             on-shell W and Z bosons, up to 300 GeV for decays via
             off-shell W and Z bosons, and up to 190 GeV for decays via
             W and Standard Model Higgs bosons.},
   Doi = {10.1140/epjc/s10052-021-09749-7},
   Key = {fds361169}
}

@article{fds307639,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for contact interactions and large extra dimensions
             in dilepton events from pp collisions at √s=7 TeV with the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.015010},
   Abstract = {A search for nonresonant new phenomena, originating from
             either contact interactions or large extra spatial
             dimensions, has been carried out using events with two
             isolated electrons or muons. These events, produced at the
             LHC in proton-proton collisions at √s=7 TeV, were recorded
             by the ATLAS detector. The data sample, collected throughout
             2011, corresponds to an integrated luminosity of 4.9 and 5.0
             fb-1 in the e+e - and μ+μ- channels, respectively. No
             significant deviations from the Standard Model expectation
             are observed. Using a Bayesian approach, 95% confidence
             level lower limits ranging from 9.0 to 13.9 TeV are placed
             on the energy scale of ℓℓqq contact interactions in the
             left-left isoscalar model. Lower limits ranging from 2.4 to
             3.9 TeV are also set on the string scale in large extra
             dimension models. After combining these limits with results
             from a similar search in the diphoton channel, slightly more
             stringent limits are obtained.},
   Doi = {10.1103/PhysRevD.87.015010},
   Key = {fds307639}
}

@article{fds310392,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Search for contact interactions and large extra dimensions
             in the dilepton channel using proton-proton collisions at
             [Formula: see text] 8 TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {12},
   Pages = {3134},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3134-6},
   Abstract = {A search is conducted for non-resonant new phenomena in
             dielectron and dimuon final states, originating from either
             contact interactions or large extra spatial dimensions. The
             LHC 2012 proton-proton collision dataset recorded by the
             ATLAS detector is used, corresponding to 20 fb[Formula: see
             text] at [Formula: see text] = 8 TeV. The dilepton
             invariant mass spectrum is a discriminating variable in both
             searches, with the contact interaction search additionally
             utilizing the dilepton forward-backward asymmetry. No
             significant deviations from the Standard Model expectation
             are observed. Lower limits are set on the [Formula: see
             text] contact interaction scale [Formula: see text] between
             15.4 TeV and 26.3 TeV, at the 95 % credibility level. For
             large extra spatial dimensions, lower limits are set on the
             string scale [Formula: see text] between 3.2 TeV to
             5.0 TeV.},
   Doi = {10.1140/epjc/s10052-014-3134-6},
   Key = {fds310392}
}

@article{fds307731,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov,
             A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
             JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez,
             VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B},
   Title = {Search for contact interactions in dilepton events from pp
             collisions at √s=7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {712},
   Number = {1-2},
   Pages = {40-58},
   Publisher = {Elsevier BV},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.04.026},
   Abstract = {This Letter presents a search for contact interactions in
             the dielectron and dimuon channels using data from
             proton-proton collisions produced by the LHC at s=7 TeV and
             recorded by the ATLAS detector. The data sample, collected
             in 2011, corresponds to an integrated luminosity of 1.08 and
             1.21 fb-1 in the e+e- and μ+μ- channels, respectively. No
             significant deviations from the standard model are observed.
             Using a Bayesian approach with a prior flat in 1/Λ2, the
             following 95% CL lower limits are placed on the energy scale
             of ℓℓqq contact interactions: Λ-&gt;10.1 TeV
             (Λ+&gt;9.4 TeV) in the electron channel and Λ-&gt;8.0 TeV
             (Λ+&gt;7.0 TeV) in the muon channel for constructive
             (destructive) interference in the left-left isoscalar
             contact interaction model. Limits are also provided for a
             prior flat in 1/Λ4. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.04.026},
   Key = {fds307731}
}

@article{fds307866,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S},
   Title = {Search for contact interactions in dimuon events from pp
             collisions at √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {84},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.011101},
   Abstract = {A search for contact interactions has been performed using
             dimuon events recorded with the ATLAS detector in
             proton-proton collisions at √s=7TeV. The data sample
             corresponds to an integrated luminosity of 42pb-1. No
             significant deviation from the standard model is observed in
             the dimuon mass spectrum, allowing the following 95% C.L.
             limits to be set on the energy scale of contact
             interactions: Λ>4.9TeV (4.5 TeV) for constructive
             (destructive) interference in the left-left isoscalar
             compositeness model. These limits are the most stringent to
             date for μμqq contact interactions. 2011 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.84.011101},
   Key = {fds307866}
}

@article{fds356704,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for dark matter and other new phenomena in events
             with an energetic jet and large missing transverse momentum
             using the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {1},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2018)126},
   Abstract = {Results of a search for new phenomena in final states with
             an energetic jet and large missing transverse momentum are
             reported. The search uses proton-proton collision data
             corresponding to an integrated luminosity of 36.1 fb−1 at
             a centre-of-mass energy of 13 TeV collected in 2015 and 2016
             with the ATLAS detector at the Large Hadron Collider. Events
             are required to have at least one jet with a transverse
             momentum above 250 GeV and no leptons (e or μ). Several
             signal regions are considered with increasing requirements
             on the missing transverse momentum above 250 GeV. Good
             agreement is observed between the number of events in data
             and Standard Model predictions. The results are translated
             into exclusion limits in models with pair-produced weakly
             interacting dark-matter candidates, large extra spatial
             dimensions, and supersymmetric particles in several
             compressed scenarios.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP01(2018)126},
   Key = {fds356704}
}

@article{fds347505,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Aubry, L and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani, H and Baines,
             JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz,
             T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black,
             KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Search for dark matter at [Formula: see text] in final
             states containing an energetic photon and large missing
             transverse momentum with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {6},
   Pages = {393},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4965-8},
   Abstract = {Results of a search for physics beyond the Standard Model in
             events containing an energetic photon and large missing
             transverse momentum with the ATLAS detector at the Large
             Hadron Collider are reported. As the number of events
             observed in data, corresponding to an integrated luminosity
             of 36.1 fb[Formula: see text]  of proton-proton collisions
             at a centre-of-mass energy of [Formula: see text], is in
             agreement with the Standard Model expectations,
             model-independent limits are set on the fiducial cross
             section for the production of events in this final state.
             Exclusion limits are also placed in models where dark-matter
             candidates are pair-produced. For dark-matter production via
             an axial-vector or a vector mediator in the
             <i>s</i>-channel, this search excludes mediator masses below
             750-[Formula: see text] for dark-matter candidate masses
             below 230-[Formula: see text] at 95% confidence level,
             depending on the couplings. In an effective theory of
             dark-matter production, the limits restrict the value of the
             suppression scale [Formula: see text] to be above [Formula:
             see text] at 95% confidence level. A limit is also reported
             on the production of a high-mass scalar resonance by
             processes beyond the Standard Model, in which the resonance
             decays to [Formula: see text] and the <i>Z</i> boson
             subsequently decays into neutrinos.},
   Doi = {10.1140/epjc/s10052-017-4965-8},
   Key = {fds347505}
}

@article{fds307652,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim,
             A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for dark matter candidates and large extra dimensions
             in events with a jet and missing transverse momentum with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {4},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2013)075},
   Abstract = {A search for new phenomena in events with a high-energy jet
             and large missing transverse momentum is performed using
             data from proton-proton collisions at √s=7 TeV with the
             ATLAS experiment at the Large Hadron Collider. Four
             kinematic regions are explored using a dataset corresponding
             to an integrated luminosity of 4.7 fb-1. No excess of events
             beyond expectations from Standard Model processes is
             observed, and limits are set on large extra dimensions and
             the pair production of dark matter particles. © 2013 CERN,
             for the benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP04(2013)075},
   Key = {fds307652}
}

@article{fds307640,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
             DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon,
             P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi,
             M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
             T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC},
   Title = {Search for dark matter candidates and large extra dimensions
             in events with a photon and missing transverse momentum in
             pp collision data at sqrt[s]=7 TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {1},
   Pages = {011802},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.110.011802},
   Abstract = {Results of a search for new phenomena in events with an
             energetic photon and large missing transverse momentum in
             proton-proton collisions at sqrt[s] = 7 TeV are reported.
             Data collected by the ATLAS experiment at the LHC
             corresponding to an integrated luminosity of 4.6 fb(-1) are
             used. Good agreement is observed between the data and the
             standard model predictions. The results are translated into
             exclusion limits on models with large extra spatial
             dimensions and on pair production of weakly interacting dark
             matter candidates.},
   Doi = {10.1103/physrevlett.110.011802},
   Key = {fds307640}
}

@article{fds356759,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Search for dark matter in association with a Higgs boson
             decaying to b-quarks in pp collisions at √s = 13 TeV with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {765},
   Pages = {11-31},
   Year = {2017},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.11.035},
   Abstract = {A search for dark matter pair production in association with
             a Higgs boson decaying to a pair of bottom quarks is
             presented, using 3.2 fb−1 of pp collisions at a
             centre-of-mass energy of 13 TeV collected by the ATLAS
             detector at the LHC. The decay of the Higgs boson is
             reconstructed as a high-momentum bb¯ system with either a
             pair of small-radius jets, or a single large-radius jet with
             substructure. The observed data are found to be consistent
             with the expected backgrounds. Results are interpreted using
             a simplified model with a Z′ gauge boson mediating the
             interaction between dark matter and the Standard Model as
             well as a two-Higgs-doublet model containing an additional
             Z′ boson which decays to a Standard Model Higgs boson and
             a new pseudoscalar Higgs boson, the latter decaying into a
             pair of dark matter particles.},
   Doi = {10.1016/j.physletb.2016.11.035},
   Key = {fds356759}
}

@article{fds356716,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
             LJ},
   Title = {Search for dark matter in association with a Higgs boson
             decaying to two photons at √s=13 TeV with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {96},
   Number = {11},
   Year = {2017},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.96.112004},
   Abstract = {A search for dark matter in association with a Higgs boson
             decaying to two photons is presented. This study is based on
             data collected with the ATLAS detector, corresponding to an
             integrated luminosity of 36.1 fb-1 of proton-proton
             collisions at the LHC at a center-of-mass energy of 13 TeV
             in 2015 and 2016. No significant excess over the expected
             background is observed. Upper limits at 95% confidence level
             are set on the visible cross section for beyond the Standard
             Model physics processes, and the production cross section
             times branching fraction of the Standard Model Higgs boson
             decaying into two photons in association with missing
             transverse momentum in three different benchmark models.
             Limits at 95% confidence level are also set on the observed
             signal in two-dimensional mass planes. Additionally, the
             results are interpreted in terms of 90% confidence-level
             limits on the dark-matter-nucleon scattering cross section,
             as a function of the dark-matter particle mass, for a
             spin-independent scenario.},
   Doi = {10.1103/PhysRevD.96.112004},
   Key = {fds356716}
}

@article{fds355555,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R},
   Title = {Search for dark matter in association with an energetic
             photon in pp collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {2},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP02(2021)226},
   Abstract = {A search for dark matter is conducted in final states
             containing a photon and missing transverse momentum in
             proton-proton collisions at s = 13 TeV. The data, collected
             during 2015–2018 by the ATLAS experiment at the CERN LHC,
             correspond to an integrated luminosity of 139 fb−1. No
             deviations from the predictions of the Standard Model are
             observed and 95% confidence-level upper limits between 2.45
             fb and 0.5 fb are set on the visible cross section for
             contributions from physics beyond the Standard Model, in
             different ranges of the missing transverse momentum. The
             results are interpreted as 95% confidence-level limits in
             models where weakly interacting dark-matter candidates are
             pair-produced via an s-channel axial-vector or vector
             mediator. Dark-matter candidates with masses up to 415 (580)
             GeV are excluded for axial-vector (vector) mediators, while
             the maximum excluded mass of the mediator is 1460 (1470)
             GeV. In addition, the results are expressed in terms of 95%
             confidence-level limits on the parameters of a model with an
             axion-like particle produced in association with a photon,
             and are used to constrain the coupling gaZγ of an
             axion-like particle to the electroweak gauge bosons. [Figure
             not available: see fulltext.]},
   Doi = {10.1007/JHEP02(2021)226},
   Key = {fds355555}
}

@article{fds356658,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
             Pereira, R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H},
   Title = {Search for dark matter in events with a hadronically
             decaying vector boson and missing transverse momentum in pp
             collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {10},
   Year = {2018},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2018)180},
   Abstract = {A search for dark matter (DM) particles produced in
             association with a hadronically decaying vector boson is
             performed using pp collision data at a centre-of-mass energy
             of s=13 TeV corresponding to an integrated luminosity of
             36.1 fb−1, recorded by the ATLAS detector at the Large
             Hadron Collider. This analysis improves on previous searches
             for processes with hadronic decays of W and Z bosons in
             association with large missing transverse momentum (mono-W/Z
             searches) due to the larger dataset and further optimization
             of the event selection and signal region definitions. In
             addition to the mono-W/Z search, the as yet unexplored
             hypothesis of a new vector boson Z′ produced in
             association with dark matter is considered (mono-Z′
             search). No significant excess over the Standard Model
             prediction is observed. The results of the mono-W/Z search
             are interpreted in terms of limits on invisible Higgs boson
             decays into dark matter particles, constraints on the
             parameter space of the simplified vector-mediator model and
             generic upper limits on the visible cross sections for
             W/Z+DM production. The results of the mono-Z′ search are
             shown in the framework of several simplified-model scenarios
             involving DM production in association with the Z′
             boson.[Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP10(2018)180},
   Key = {fds356658}
}

@article{fds307552,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
             E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernhard, R and Bernius, C and Bernlochner,
             FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
             MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao
             De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
             V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
             J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
             P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger,
             K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Buehrer, F and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
             B and Chapman, JD and Chapman, JW and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov,
             A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow,
             BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba,
             J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron,
             ZH},
   Title = {Search for dark matter in events with a hadronically
             decaying W or Z boson and missing transverse momentum in pp
             collisions at √s=8  TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {4},
   Pages = {041802},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.112.041802},
   Abstract = {A search is presented for dark matter pair production in
             association with a W or Z boson in pp collisions
             representing 20.3  fb(-1) of integrated luminosity at
             √s=8  TeV using data recorded with the ATLAS detector
             at the Large Hadron Collider. Events with a hadronic jet
             with the jet mass consistent with a W or Z boson, and with
             large missing transverse momentum are analyzed. The data are
             consistent with the standard model expectations. Limits are
             set on the mass scale in effective field theories that
             describe the interaction of dark matter and standard model
             particles, and on the cross section of Higgs production and
             decay to invisible particles. In addition, cross section
             limits on the anomalous production of W or Z bosons with
             large missing transverse momentum are set in two fiducial
             regions.},
   Doi = {10.1103/physrevlett.112.041802},
   Key = {fds307552}
}

@article{fds310373,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for dark matter in events with a Z boson and missing
             transverse momentum in pp collisions at s =8TeV with the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.012004},
   Abstract = {A search is presented for production of dark-matter
             particles recoiling against a leptonically decaying Z boson
             in 20.3fb-1 of pp collisions at s=8TeV with the ATLAS
             detector at the Large Hadron Collider. Events with large
             missing transverse momentum and two oppositely charged
             electrons or muons consistent with the decay of a Z boson
             are analyzed. No excess above the Standard Model prediction
             is observed. Limits are set on the mass scale of the contact
             interaction as a function of the dark-matter particle mass
             using an effective field theory description of the
             interaction of dark matter with quarks or with Z bosons.
             Limits are also set on the coupling and mediator mass of a
             model in which the interaction is mediated by a scalar
             particle. © 2014 CERN, for the ATLAS Collaboration.},
   Doi = {10.1103/PhysRevD.90.012004},
   Key = {fds310373}
}

@article{fds310316,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, M and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
             M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Azuma, Y and Baak, MA and Baas,
             AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus,
             M and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov,
             SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Battistin, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie,
             MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck,
             HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
             FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci,
             F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
             CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
             V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron,
             J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
             AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan,
             JG},
   Title = {Search for dark matter in events with heavy quarks and
             missing transverse momentum in [Formula: see text]
             collisions with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {2},
   Pages = {92},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3306-z},
   Abstract = {This article reports on a search for dark matter pair
             production in association with bottom or top quarks in
             [Formula: see text] of [Formula: see text] collisions
             collected at [Formula: see text] TeV by the ATLAS detector
             at the LHC. Events with large missing transverse momentum
             are selected when produced in association with high-momentum
             jets of which one or more are identified as jets containing
             [Formula: see text]-quarks. Final states with top quarks are
             selected by requiring a high jet multiplicity and in some
             cases a single lepton. The data are found to be consistent
             with the Standard Model expectations and limits are set on
             the mass scale of effective field theories that describe
             scalar and tensor interactions between dark matter and
             Standard Model particles. Limits on the dark-matter-nucleon
             cross-section for spin-independent and spin-dependent
             interactions are also provided. These limits are
             particularly strong for low-mass dark matter. Using a
             simplified model, constraints are set on the mass of dark
             matter and of a coloured mediator suitable to explain a
             possible signal of annihilating dark matter.},
   Doi = {10.1140/epjc/s10052-015-3306-z},
   Key = {fds310316}
}

@article{fds313602,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
             P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
             S},
   Title = {Search for Dark Matter in Events with Missing Transverse
             Momentum and a Higgs Boson Decaying to Two Photons in pp
             Collisions at sqrt[s]=8 TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {115},
   Number = {13},
   Pages = {131801},
   Year = {2015},
   Month = {September},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.115.131801},
   Abstract = {Results of a search for new phenomena in events with large
             missing transverse momentum and a Higgs boson decaying to
             two photons are reported. Data from proton-proton collisions
             at a center-of-mass energy of 8 TeV and corresponding to an
             integrated luminosity of 20.3 fb^{-1} have been collected
             with the ATLAS detector at the LHC. The observed data are
             well described by the expected standard model backgrounds.
             Upper limits on the cross section of events with large
             missing transverse momentum and a Higgs boson candidate are
             also placed. Exclusion limits are presented for models of
             physics beyond the standard model featuring dark-matter
             candidates.},
   Doi = {10.1103/physrevlett.115.131801},
   Key = {fds313602}
}

@article{fds307703,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Bai,
             Y and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Fox, PJ and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harnik, R and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins,
             W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon,
             T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, C and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys,
             J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paus, C and Pellett,
             DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Search for dark matter in events with one jet and missing
             transverse energy in pp¯ collisions at √s=1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {21},
   Pages = {211804},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.211804},
   Abstract = {We present the results of a search for dark matter
             production in the monojet signature. We analyze a sample of
             Tevatron pp[over ¯] collisions at √s=1.96 TeV
             corresponding to an integrated luminosity of 6.7 fb(-1)
             recorded by the CDF II detector. In events with large
             missing transverse energy and one energetic jet, we find
             good agreement between the standard model prediction and the
             observed data. We set 90% confidence level upper limits on
             the dark matter production rate. The limits are translated
             into bounds on nucleon-dark matter scattering rates which
             are competitive with current direct detection bounds on
             spin-independent interaction below a dark matter candidate
             mass of 5 GeV/c(2), and on spin-dependent interactions up to
             masses of 200 GeV/c(2).},
   Doi = {10.1103/physrevlett.108.211804},
   Key = {fds307703}
}

@article{fds356025,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith,
             L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten,
             K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis,
             C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji,
             S and Balasubramanian, R and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton,
             AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso,
             MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
             F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia
             Bylund, O and Besson, N and Bethke, S and Betti, A and Bevan, AJ and Beyer,
             J and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman,
             M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich,
             C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla,
             JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska,
             HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
             JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner,
             L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr,
             JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti,
             P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capua, M and Cardarelli,
             R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carratta, G and Carter, JWS and Carter,
             TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, YS and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Chytka, L and Cieri, D},
   Title = {Search for Dark Matter Produced in Association with a Dark
             Higgs Boson Decaying into W^{±}W^{∓} or ZZ in Fully
             Hadronic Final States from sqrt[s]=13  TeV pp Collisions
             Recorded with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {126},
   Number = {12},
   Pages = {121802},
   Year = {2021},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.126.121802},
   Abstract = {Several extensions of the Standard Model predict the
             production of dark matter particles at the LHC. An uncharted
             signature of dark matter particles produced in association
             with VV=W^{±}W^{∓} or ZZ pairs from a decay of a dark
             Higgs boson s is searched for using 139  fb^{-1} of pp
             collisions recorded by the ATLAS detector at a
             center-of-mass energy of 13 TeV. The s→V(qq[over
             ¯])V(qq[over ¯]) decays are reconstructed with a novel
             technique aimed at resolving the dense topology from boosted
             VV pairs using jets in the calorimeter and tracking
             information. Dark Higgs scenarios with m_{s}>160  GeV
             are excluded.},
   Doi = {10.1103/physrevlett.126.121802},
   Key = {fds356025}
}

@article{fds321071,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for dark matter produced in association with a
             hadronically decaying vector boson in pp collisions at
             √s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {763},
   Pages = {251-268},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.10.042},
   Abstract = {A search is presented for dark matter produced in
             association with a hadronically decaying W or Z boson using
             3.2 fb−1 of pp collisions at s=13 TeV recorded by the
             ATLAS detector at the Large Hadron Collider. Events with a
             hadronic jet compatible with a W or Z boson and with large
             missing transverse momentum are analysed. The data are
             consistent with the Standard Model predictions and are
             interpreted in terms of both an effective field theory and a
             simplified model containing dark matter.},
   Doi = {10.1016/j.physletb.2016.10.042},
   Key = {fds321071}
}

@article{fds329964,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines,
             JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann,
             TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
             NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
             TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark,
             MR},
   Title = {Search for Dark Matter Produced in Association with a Higgs
             Boson Decaying to bb[over ¯] Using 36  fb^{-1} of pp
             Collisions at sqrt[s]=13  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {119},
   Number = {18},
   Pages = {181804},
   Year = {2017},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.119.181804},
   Abstract = {Several extensions of the standard model predict associated
             production of dark-matter particles with a Higgs boson. Such
             processes are searched for in final states with missing
             transverse momentum and a Higgs boson decaying to a bb[over
             ¯] pair with the ATLAS detector using 36.1  fb^{-1} of
             pp collisions at a center-of-mass energy of 13 TeV at the
             LHC. The observed data are in agreement with the standard
             model predictions and limits are placed on the associated
             production of dark-matter particles and a Higgs
             boson.},
   Doi = {10.1103/physrevlett.119.181804},
   Key = {fds329964}
}

@article{fds315364,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Search for dark matter produced in association with a Higgs
             boson decaying to two bottom quarks in pp collisions at s =8
             TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {April},
   ISSN = {2470-0010},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.072007},
   Abstract = {This article reports on a search for dark matter pair
             production in association with a Higgs boson decaying to a
             pair of bottom quarks, using data from 20.3 fb-1 of pp
             collisions at a center-of-mass energy of 8 TeV collected by
             the ATLAS detector at the LHC. The decay of the Higgs boson
             is reconstructed as a high-momentum bb system with either a
             pair of small-radius jets, or a single large-radius jet with
             substructure. The observed data are found to be consistent
             with the expected Standard Model backgrounds.
             Model-independent upper limits are placed on the visible
             cross sections for events with a Higgs boson decaying into
             bb and large missing transverse momentum with thresholds
             ranging from 150 to 400 GeV. Results are interpreted using a
             simplified model with a Z′ gauge boson decaying into
             different Higgs bosons predicted in a two-Higgs-doublet
             model, of which the heavy pseudoscalar Higgs decays into a
             pair of dark matter particles. Exclusion limits are also
             presented for the mass scales of various effective field
             theory operators that describe the interaction between dark
             matter particles and the Higgs boson.},
   Doi = {10.1103/PhysRevD.93.072007},
   Key = {fds315364}
}

@article{fds374253,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
             CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
             P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
             C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev,
             V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
             JF},
   Title = {Search for dark matter produced in association with a single
             top quark and an energetic W boson in √s= 13 TeV pp
             collisions with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {7},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2023},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11582-z},
   Abstract = {This paper presents a search for dark matter, χ , using
             events with a single top quark and an energetic W boson. The
             analysis is based on proton–proton collision data
             collected with the ATLAS experiment at s= 13 TeV during LHC
             Run 2 (2015–2018), corresponding to an integrated
             luminosity of 139 fb - 1 . The search considers final states
             with zero or one charged lepton (electron or muon), at least
             one b-jet and large missing transverse momentum. In
             addition, a result from a previous search considering
             two-charged-lepton final states is included in the
             interpretation of the results. The data are found to be in
             good agreement with the Standard Model predictions and the
             results are interpreted in terms of 95% confidence-level
             exclusion limits in the context of a class of dark matter
             models involving an extended two-Higgs-doublet sector
             together with a pseudoscalar mediator particle. The search
             is particularly sensitive to on-shell production of the
             charged Higgs boson state, H± , arising from the
             two-Higgs-doublet mixing, and its semi-invisible decays via
             the mediator particle, a: H±→ W±a(→ χχ) . Signal
             models with H± masses up to 1.5 TeV and a masses up to 350
             GeV are excluded assuming a tan β value of 1. For masses of
             a of 150 (250) GeV, tan β values up to 2 are excluded for
             H± masses between 200 (400) GeV and 1.5 TeV. Signals with
             tan β values between 20 and 30 are excluded for H± masses
             between 500 and 800 GeV.},
   Doi = {10.1140/epjc/s10052-023-11582-z},
   Key = {fds374253}
}

@article{fds359540,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
             M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
   Title = {Search for dark matter produced in association with a single
             top quark in √s=13 TeV pp collisions with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {10},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09566-y},
   Abstract = {This paper presents a search for dark matter in the context
             of a two-Higgs-doublet model together with an additional
             pseudoscalar mediator, a, which decays into the dark-matter
             particles. Processes where the pseudoscalar mediator is
             produced in association with a single top quark in the
             2HDM+a model are explored for the first time at the LHC.
             Several final states which include either one or two charged
             leptons (electrons or muons) and a significant amount of
             missing transverse momentum are considered. The analysis is
             based on proton–proton collision data collected with the
             ATLAS experiment at s=13 TeV during LHC Run 2
             (2015–2018), corresponding to an integrated luminosity of
             139 fb - 1. No significant excess above the Standard Model
             predictions is found. The results are expressed as 95%
             confidence-level limits on the parameters of the signal
             models considered.},
   Doi = {10.1140/epjc/s10052-021-09566-y},
   Key = {fds359540}
}

@article{fds360568,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S},
   Title = {Search for dark matter produced in association with a
             Standard Model Higgs boson decaying into b-quarks using the
             full Run 2 dataset from the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {11},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2021)209},
   Abstract = {The production of dark matter in association with Higgs
             bosons is predicted in several extensions of the Standard
             Model. An exploration of such scenarios is presented,
             considering final states with missing transverse momentum
             and b-tagged jets consistent with a Higgs boson. The
             analysis uses proton-proton collision data at a
             centre-of-mass energy of 13 TeV recorded by the ATLAS
             experiment at the LHC during Run 2, amounting to an
             integrated luminosity of 139 fb−1. The analysis, when
             compared with previous searches, benefits from a larger
             dataset, but also has further improvements providing
             sensitivity to a wider spectrum of signal scenarios. These
             improvements include both an optimised event selection and
             advances in the object identification, such as the use of
             the likelihood-based significance of the missing transverse
             momentum and variable-radius track-jets. No significant
             deviation from Standard Model expectations is observed.
             Limits are set, at 95% confidence level, in two benchmark
             models with two Higgs doublets extended by either a heavy
             vector boson Z′ or a pseudoscalar singlet a and which both
             provide a dark matter candidate χ. In the case of the
             two-Higgs-doublet model with an additional vector boson
             Z′, the observed limits extend up to a Z′ mass of 3 TeV
             for a mass of 100 GeV for the dark matter candidate. The
             two-Higgs-doublet model with a dark matter particle mass of
             10 GeV and an additional pseudoscalar a is excluded for
             masses of the a up to 520 GeV and 240 GeV for tan β = 1 and
             tan β = 10 respectively. Limits on the visible
             cross-sections are set and range from to 0.05 fb to 3.26 fb,
             depending on the missing transverse momentum and b-quark jet
             multiplicity requirements. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP11(2021)209},
   Key = {fds360568}
}

@article{fds347464,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
             H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
             O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Changqiao, C-Q and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba,
             LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo,
             F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati,
             L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
             YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
             YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Search for dark matter produced in association with bottom
             or top quarks in s = 13  TeV pp collisions with the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {1},
   Pages = {18},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5486-1},
   Abstract = {A search for weakly interacting massive dark-matter
             particles produced in association with bottom or top quarks
             is presented. Final states containing third-generation
             quarks and missing transverse momentum are considered. The
             analysis uses 36.1 fb - 1 of proton-proton collision data
             recorded by the ATLAS experiment at s = 13  TeV in 2015 and
             2016. No significant excess of events above the estimated
             backgrounds is observed. The results are interpreted in the
             framework of simplified models of spin-0 dark-matter
             mediators. For colour-neutral spin-0 mediators produced in
             association with top quarks and decaying into a pair of
             dark-matter particles, mediator masses below 50 GeV are
             excluded assuming a dark-matter candidate mass of 1 GeV and
             unitary couplings. For scalar and pseudoscalar mediators
             produced in association with bottom quarks, the search sets
             limits on the production cross-section of 300 times the
             predicted rate for mediators with masses between 10 and 50
             GeV and assuming a dark-matter mass of 1 GeV and unitary
             coupling. Constraints on colour-charged scalar simplified
             models are also presented. Assuming a dark-matter particle
             mass of 35 GeV , mediator particles with mass below 1.1 TeV
             are excluded for couplings yielding a dark-matter relic
             density consistent with measurements.},
   Doi = {10.1140/epjc/s10052-017-5486-1},
   Key = {fds347464}
}

@article{fds375226,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
             J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
             Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
             GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
             M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
             JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
             Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
             PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour,
             G and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr,
             AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
             M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano
             Hurrell, LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
             F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov,
             VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
             M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir,
             M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal,
             J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
             R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
             PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
             CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo
             Vazquez, CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir,
             O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
             Bret, M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone,
             A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin,
             E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo,
             FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
             J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
             A},
   Title = {Search for Dark Photons in Rare Z Boson Decays with the
             ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {131},
   Number = {25},
   Pages = {251801},
   Year = {2023},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.131.251801},
   Abstract = {A search for events with a dark photon produced in
             association with a dark Higgs boson via rare decays of the
             standard model Z boson is presented, using 139  fb^{-1}
             of sqrt[s]=13  TeV proton-proton collision data recorded
             by the ATLAS detector at the Large Hadron Collider. The dark
             boson decays into a pair of dark photons, and at least two
             of the three dark photons must each decay into a pair of
             electrons or muons, resulting in at least two same-flavor
             opposite-charge lepton pairs in the final state. The data
             are found to be consistent with the background prediction,
             and upper limits are set on the dark photon's coupling to
             the dark Higgs boson times the kinetic mixing between the
             standard model photon and the dark photon, α_{D}ϵ^{2}, in
             the dark photon mass range of [5, 40] GeV except for the ϒ
             mass window [8.8, 11.1] GeV. This search explores new
             parameter space not previously excluded by other
             experiments.},
   Doi = {10.1103/physrevlett.131.251801},
   Key = {fds375226}
}

@article{fds307824,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Aktas, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {Search for decays of stopped, long-lived particles from 7
             TeV pp collisions with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {4},
   Pages = {1-21},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-1965-6},
   Abstract = {New metastable massive particles with electric and colour
             charge are features of many theories beyond the Standard
             Model. A search is performed for long-lived gluino-based
             R-hadrons with the ATLAS detector at the LHC using a data
             sample corresponding to an integrated luminosity of 31
             pb−1. We search for evidence of particles that have come
             to rest in the ATLAS detector and decay at some later time
             during the periods in the LHC bunch structure without
             proton–proton collisions. No significant deviations from
             the expected backgrounds are observed, and a cross-section
             limit is set. It can be interpreted as excluding
             gluino-based R-hadrons with masses less than 341 GeV at the
             95 % C.L., for lifetimes from 10−5to 103seconds and a
             neutralino mass of 100 GeV.},
   Doi = {10.1140/epjc/s10052-012-1965-6},
   Key = {fds307824}
}

@article{fds356581,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
             V},
   Title = {Search for diboson resonances in hadronic final states in
             139 fb−1 of pp collisions at √s = 13 TeV with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {9},
   Year = {2019},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2019)091},
   Abstract = {Narrow resonances decaying into W W, W Z or ZZ boson pairs
             are searched for in 139 fb−1 of proton-proton collision
             data at a centre-of-mass energy of s = 13 TeV recorded with
             the ATLAS detector at the Large Hadron Collider from 2015 to
             2018. The diboson system is reconstructed using pairs of
             high transverse momentum, large-radius jets. These jets are
             built from a combination of calorimeter- and tracker-inputs
             compatible with the hadronic decay of a boosted W or Z
             boson, using jet mass and substructure properties. The
             search is performed for diboson resonances with masses
             greater than 1.3 TeV. No significant deviations from the
             background expectations are observed. Exclusion limits at
             the 95% confidence level are set on the production
             cross-section times branching ratio into dibosons for
             resonances in a range of theories beyond the Standard Model,
             with the highest excluded mass of a new gauge boson at 3.8
             TeV in the context of mass-degenerate resonances that couple
             predominantly to gauge bosons.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP09(2019)091},
   Key = {fds356581}
}

@article{fds356697,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for diboson resonances with boson-tagged jets in pp
             collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {777},
   Pages = {91-113},
   Year = {2018},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2017.12.011},
   Abstract = {Narrow resonances decaying into WW, WZ or ZZ boson pairs are
             searched for in 36.7 fb−1 of proton–proton collision
             data at a centre-of-mass energy of s=13 TeV recorded with
             the ATLAS detector at the Large Hadron Collider in 2015 and
             2016. The diboson system is reconstructed using pairs of
             large-radius jets with high transverse momentum and tagged
             as compatible with the hadronic decay of high-momentum W or
             Z bosons, using jet mass and substructure properties. The
             search is sensitive to diboson resonances with masses in the
             range 1.2–5.0 TeV. No significant excess is observed in
             any signal region. Exclusion limits are set at the 95%
             confidence level on the production cross section times
             branching ratio to dibosons for a range of theories beyond
             the Standard Model. Model-dependent lower limits on the mass
             of new gauge bosons are set, with the highest limit set at
             3.5 TeV in the context of mass-degenerate resonances that
             couple predominantly to bosons.},
   Doi = {10.1016/j.physletb.2017.12.011},
   Key = {fds356697}
}

@article{fds351558,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH},
   Title = {Search for dijet resonances in events with an isolated
             charged lepton using √s = 13 TeV proton-proton collision
             data collected by the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {6},
   Year = {2020},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2020)151},
   Abstract = {A search for dijet resonances in events with at least one
             isolated charged lepon is performed using 139 fb−1 of s =
             13 TeV proton-proton collision data recorded by the ATLAS
             detector at the LHC. The dijet invariant-mass (mjj)
             distribution constructed from events with at least one
             isolated electron or muon is searched in the region 0.22 <
             mjj< 6.3 TeV for excesses above a smoothly falling
             background from Standard Model processes. Triggering based
             on the presence of a lepton in the event reduces limitations
             imposed by minimum transverse momentum thresholds for
             triggering on jets. This approach allows smaller dijet
             invariant masses to be probed than in inclusive dijet
             searches, targeting a variety of new-physics models, for
             example ones in which a new state is produced in association
             with a leptonically decaying W or Z boson. No statistically
             significant deviation from the Standard Model background
             hypothesis is found. Limits on contributions from generic
             Gaussian signals with widths ranging from that determined by
             the detector resolution up to 15% of the resonance mass are
             obtained for dijet invariant masses ranging from 0.25 TeV to
             6 TeV. Limits are set also in the context of several
             scenarios beyond the Standard Model, such as the Sequential
             Standard Model, a technicolor model, a charged Higgs boson
             model and a simplified Dark Matter model. [Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP06(2020)151},
   Key = {fds351558}
}

@article{fds307826,
   Author = {Collaboration, AVKWGAEAATLAS},
   Title = {Search for dilepton resonances in pp collisions at 7 TeV
             with the ATLAS detector},
   Journal = {Physical Review Letters},
   Volume = {107},
   Number = {27},
   Pages = {272002},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.107.272002},
   Abstract = {This Letter reports on a search for narrow high-mass
             resonances decaying into dilepton final states. The data
             were recorded by the ATLAS experiment in pp collisions at
             √s=7  TeV at the Large Hadron Collider and correspond
             to a total integrated luminosity of 1.08 (1.21)  fb(-1)
             in the e(+)e(-) (μ(+)μ(-)) channel. No statistically
             significant excess above the standard model expectation is
             observed and upper limits are set at the 95% C.L. on the
             cross section times branching fraction of Z' resonances and
             Randall-Sundrum gravitons decaying into dileptons as a
             function of the resonance mass. A lower mass limit of 1.83
             TeV on the sequential standard model Z' boson is set. A
             Randall-Sundrum graviton with coupling k/M(Pl)=0.1 is
             excluded at 95% C.L. for masses below 1.63
             TeV.},
   Doi = {10.1103/physrevlett.107.272002},
   Key = {fds307826}
}

@article{fds332355,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
             JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
             R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
             D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MAC and Cutts,
             D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann,
             R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
             OV},
   Title = {Search for dilepton signatures from minimal low-energy
             supergravity in [Formula Presented] collisions at [Formula
             Presented] TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {63},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2001},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.63.091102},
   Abstract = {We report on a search for supersymmetry using the DØ
             detector. The 1994–1996 data sample of [Formula Presented]
             TeV [Formula Presented] collisions was analyzed for events
             containing two leptons [Formula Presented] or [Formula
             Presented] two or more jets, and missing transverse energy.
             Assuming the minimal supergravity model, with [Formula
             Presented] and [Formula Presented] various thresholds were
             employed to optimize the search. No events were found beyond
             expectation from the background. We set a lower limit at the
             95% C.L. of 255 [Formula Presented] for equal mass squarks
             and gluinos for [Formula Presented] and present exclusion
             contours in the [Formula Presented] plane for [Formula
             Presented]–6. © 2001 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.63.091102},
   Key = {fds332355}
}

@booklet{Abachi97f,
   Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Álvarez, G and Alves,
             GA and Amidi, E and Amos, N and Anderson, EW and Aronson, SH and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Bendich, J and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Bischoff, A and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt,
             A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty,
             D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
             C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and De,
             K and Del-Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard,
             J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahey, S and Fahland, T and Fatyga, M and Fatyga, MK and Featherly, J and Feher, S},
   Title = {Search for diphoton events with large missing transverse
             energy in pp collisions at = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {78},
   Number = {11},
   Pages = {2070-2074},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.78.2070},
   Abstract = {A search for new physics has been carried out in the channel
             pp → γγ + ET, as expected in various supersymmetric
             models. We require two photons with transverse energy EγT >
             12 GeV and pseudorapidity |ηγ < 1.1. The distribution of
             missing transverse energy (ET) is consistent with background
             and no events have ET > 25 GeV. We set limits on production
             cross sections for selectron, sneutrino, and neutralino
             pairs, decaying into photons, which range from about 400 fb
             to 1 pb depending on the sparticle masses. A general limit
             of 185 fb (95% C.L.) is set on σ(pp → γγET + X), where
             eγT > 12 GeV, |ηγ| < 1.1, and ET > 25 GeV. © 1997 The
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.78.2070},
   Key = {Abachi97f}
}

@article{fds307836,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Search for diphoton events with large missing transverse
             energy with 36 pb-1 of 7 TeV proton-proton
             collision data with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1744-9},
   Abstract = {Making use of 36 pb-1 of proton-proton collision data at
             √s = 7 TeV, the ATLAS Collaboration has performed a search
             for diphoton events with large missing transverse energy.
             Observing no excess of events above the Standard Model
             prediction, a 95% Confidence Level (CL) upper limit is set
             on the cross section for new physics of σ < 0.38-0.65 pb in
             the context of a generalised model of gauge-mediated
             supersymmetry breaking (GGM) with a bino-like lightest
             neutralino, and of σ < 0.18-0.23 pb in the context of a
             specific model with one universal extra dimension (UED). A
             95% CL lower limit of 560 GeV, for bino masses above 50 GeV,
             is set on the GGM gluino mass, while a lower limit of 1/R >
             961 GeV is set on the UED compactification radius R. These
             limits provide the most stringent tests of these models to
             date.},
   Doi = {10.1140/epjc/s10052-011-1744-9},
   Key = {fds307836}
}

@article{fds307761,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
             G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, SW and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart,
             H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
             R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan,
             M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG},
   Title = {Search for diphoton events with large missing transverse
             momentum in 1 fb -1 of 7 TeV proton-proton
             collision data with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {710},
   Number = {4-5},
   Pages = {519-537},
   Publisher = {Elsevier BV},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.054},
   Abstract = {A search for diphoton events with large missing transverse
             momentum has been performed using 1.07 fb -1 of
             proton-proton collision data at s=7 TeV recorded with the
             ATLAS detector. No excess of events was observed above the
             Standard Model prediction and 95% Confidence Level (CL)
             upper limits are set on the production cross section for new
             physics. The limits depend on each model parameter space and
             vary as follows: Λ&lt;(22-129) fb in the context of a
             generalised model of gauge-mediated supersymmetry breaking
             (GGM) with a bino-like lightest neutralino, σ&lt;(27-91) fb
             in the context of a minimal model of gauge-mediated
             supersymmetry breaking (SPS8), and σ&lt;(15-27) fb in the
             context of a specific model with one universal extra
             dimension (UED). A 95% CL lower limit of 805 GeV, for bino
             masses above 50 GeV, is set on the GGM gluino mass. Lower
             limits of 145 TeV and 1.23 TeV are set on the SPS8 breaking
             scale Λ and on the UED compactification scale 1/R,
             respectively. These limits provide the most stringent tests
             of these models to date. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.02.054},
   Key = {fds307761}
}

@article{fds307655,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and A°kesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Search for diphoton events with large missing transverse
             momentum in 7 TeV proton-proton collision data with the
             ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {718},
   Number = {2},
   Pages = {411-430},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {December},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.10.069},
   Abstract = {A search for diphoton events with large missing transverse
             momentum has been performed using proton-proton collision
             data at s=7 TeV recorded with the ATLAS detector,
             corresponding to an integrated luminosity of 4.8 fb-1. No
             excess of events was observed above the Standard Model
             prediction and model-dependent 95% confidence level
             exclusion limits are set. In the context of a generalised
             model of gauge-mediated supersymmetry breaking with a
             bino-like lightest neutralino of mass above 50 GeV, gluinos
             (squarks) below 1.07 TeV (0.87 TeV) are excluded, while a
             breaking scale Λ below 196 TeV is excluded for a minimal
             model of gauge-mediated supersymmetry breaking. For a
             specific model with one universal extra dimension,
             compactification scales 1/R<1.40 TeV are excluded. These
             limits provide the most stringent tests of these models to
             date. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.10.069},
   Key = {fds307655}
}

@article{fds307643,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, JF and Arik, E},
   Title = {Search for direct chargino production in anomaly-mediated
             supersymmetry breaking models based on a disappearing-track
             signature in pp collisions at √s=7TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP01(2013)131},
   Abstract = {A search for direct chargino production in anomaly-mediated
             supersymmetry breaking scenarios is performed in pp
             collisions at √s=7TeV using 4.7 fb-1 of data collected
             with the ATLAS experiment at the LHC. In these models, the
             lightest chargino is predicted to have a lifetime long
             enough to be detected in the tracking detectors of collider
             experiments. This analysis explores such models by searching
             for chargino decays that result in tracks with few
             associated hits in the outer region of the tracking system.
             The transverse-momentum spectrum of candidate tracks is
             found to be consistent with the expectation from the
             Standard Model background processes and constraints on
             chargino properties are obtained. © 2013 CERN for the
             benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP01(2013)131},
   Key = {fds307643}
}

@article{fds310320,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Beven, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C},
   Title = {Search for direct pair production of a chargino and a
             neutralino decaying to the 125 GeV Higgs boson in [Formula:
             see text] TeV [Formula: see text] collisions with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {5},
   Pages = {208},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3408-7},
   Abstract = {A search is presented for the direct pair production of a
             chargino and a neutralino [Formula: see text], where the
             chargino decays to the lightest neutralino and the [Formula:
             see text] boson, [Formula: see text], while the neutralino
             decays to the lightest neutralino and the 125 GeV Higgs
             boson, [Formula: see text]. The final states considered for
             the search have large missing transverse momentum, an
             isolated electron or muon, and one of the following: either
             two jets identified as originating from bottom quarks, or
             two photons, or a second electron or muon with the same
             electric charge. The analysis is based on 20.3 [Formula:
             see text] of [Formula: see text] proton-proton collision
             data delivered by the Large Hadron Collider and recorded
             with the ATLAS detector. Observations are consistent with
             the Standard Model expectations, and limits are set in the
             context of a simplified supersymmetric model.},
   Doi = {10.1140/epjc/s10052-015-3408-7},
   Key = {fds310320}
}

@article{fds310362,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for direct pair production of the top squark in
             all-hadronic final states in proton-proton collisions at
             √s = 8TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {9},
   Pages = {1-51},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2014)015},
   Abstract = {The results of a search for direct pair production of the
             scalar partner to the top quark using an integrated
             luminosity of 20.1 fb-1 of proton-proton collision data at
             yfs = 8 TeV recorded with the ATLAS detector at the LHC are
             reported. The top squark is assumed to decay via t → t
             χ¯01 or t → b χ1 → bW(*)χ-01, where χ-01 (x1)
             denotes the lightest neutralino (chargino) in supersymmetric
             models. The search targets a fully-hadronic final state in
             events with four or more jets and large missing transverse
             momentum. No significant excess over the Standard Model
             background prediction is observed, and exclusion limits are
             reported in terms of the top squark and neutralino masses
             and as a function of the branching fraction of t → t
             χ-01. For a branching fraction of 100%, top squark masses
             in the range 270-645 GeV are excluded for χ-01 masses below
             30GeV. For a branching fraction of 50% to either t → t
             χ-01 or t → b χ-01, and assuming the χ¯1 mass to be
             twice the χ-01 mass, top squark masses in the range 250-550
             GeV are excluded for χ-01 masses below 60
             GeV.},
   Doi = {10.1007/JHEP09(2014)015},
   Key = {fds310362}
}

@article{fds307546,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O},
   Title = {Search for direct production of charginos and neutralinos in
             events with three leptons and missing transverse momentum in
             pv s = 8 TeV pp collisions with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {4},
   Pages = {1-52},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP04(2014)169},
   Abstract = {A search for the direct production of charginos and
             neutralinos in final states with three leptons and missing
             transverse momentum is presented. The analysis is based on
             20.3 fb-1 of vs = 8TeV proton-proton collision data
             delivered by the Large Hadron Collider and recorded with the
             ATLAS detector. Observations are consistent with the
             Standard Model expectations and limits are set in
             R-parity-conserving phenomenological Minimal Supersymmetric
             Standard Models and in simplified supersymmetric models,
             significantly extending previous results. For simplified
             supersymmetric models of direct chargino (∼X±1) and
             next-to-lightest neutralino (X∼02) production with decays
             to lightest neutralino (∼X01) via either all three
             generations of sleptons, staus only, gauge bosons, or Higgs
             bosons, ∼X± 1 and ∼X02 masses are excluded up to
             700GeV, 380GeV, 345GeV, or 148GeV respectively, for a
             massless ∼X01.},
   Doi = {10.1007/JHEP04(2014)169},
   Key = {fds307546}
}

@article{fds307638,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ},
   Title = {Search for direct production of charginos and neutralinos in
             events with three leptons and missing transverse momentum in
             √s=7 TeV pp collisions with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {718},
   Number = {3},
   Pages = {841-859},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.11.039},
   Abstract = {A search for the direct production of charginos and
             neutralinos in final states with three electrons or muons
             and missing transverse momentum is presented. The analysis
             is based on 4.7 fb−1 of s=7 TeV proton–proton collision
             data delivered by the Large Hadron Collider and recorded
             with the ATLAS detector. Observations are consistent with
             Standard Model expectations in three signal regions that are
             either depleted or enriched in Z-boson decays. Upper limits
             at 95% confidence level are set in R-parity conserving
             phenomenological minimal supersymmetric models and in
             simplified models, significantly extending previous
             results.},
   Doi = {10.1016/j.physletb.2012.11.039},
   Key = {fds307638}
}

@article{fds336987,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O},
   Title = {Search for direct production of charginos, neutralinos and
             sleptons in final states with two leptons and missing
             transverse momentum in pp collisions at √s = 8TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {5},
   Pages = {1-51},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2014)071},
   Abstract = {Searches for the electroweak production of charginos,
             neutralinos and sleptons in final states characterized by
             the presence of two leptons (electrons and muons) and
             missing transverse momentum are performed using 20.3 fb-1of
             proton-proton collision data at √s = 8TeV recorded with
             the ATLAS experiment at the Large Hadron Collider. No
             significant excess beyond Standard Model expectations is
             observed. Limits are set on the masses of the lightest
             chargino, next-to-lightest neutralino and sleptons for
             different lightest-neutralino mass hypotheses in simplified
             models. Results are also interpreted in various scenarios of
             the phenomenological Minimal Supersymmetric Standard
             Model.},
   Doi = {10.1007/JHEP05(2014)071},
   Key = {fds336987}
}

@article{fds352892,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
             Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V},
   Title = {Search for direct production of electroweakinos in final
             states with missing transverse momentum and a Higgs boson
             decaying into photons in pp collisions at √s = 13 TeV with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {10},
   Year = {2020},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2020)005},
   Abstract = {A search for a chargino-neutralino pair decaying via the 125
             GeV Higgs boson into photons is presented. The study is
             based on the data collected between 2015 and 2018 with the
             ATLAS detector at the LHC, corresponding to an integrated
             luminosity of 139 fb−1 of pp collisions at a
             centre-of-mass energy of 13 TeV. No significant excess over
             the expected background is observed. Upper limits at 95%
             confidence level for a massless χ˜10 are set on several
             electroweakino production cross-sections and the visible
             cross-section for beyond the Standard Model processes. In
             the context of simplified supersymmetric models, 95%
             confidence-level limits of up to 310 GeV in
             m(χ˜1±/χ˜20), where m(χ˜10) = 0.5 GeV, are set.
             Limits at 95% confidence level are also set on the
             χ˜1±χ˜20 cross-section in the mass plane of
             m(χ˜1±/χ˜20) and m(χ˜10), and on scenarios with
             gravitino as the lightest supersymmetric particle. Upper
             limits at the 95% confidence-level are set on the higgsino
             production cross-section. Higgsino masses below 380 GeV are
             excluded for the case of the higgsino fully decaying into a
             Higgs boson and a gravitino. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP10(2020)005},
   Key = {fds352892}
}

@article{fds351473,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abulaiti, Y and Abreu, H and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Pozo, JAA and Bella, LA and Arabidze, G},
   Title = {Search for direct production of electroweakinos in final
             states with one lepton, missing transverse momentum and a
             Higgs boson decaying into two b-jets in pp collisions at
             √s=13 TeV with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {8},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2020},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-8050-3},
   Abstract = {The results of a search for electroweakino pair production
             pp→χ~1±χ~20 in which the chargino (χ~1±) decays into
             a W boson and the lightest neutralino (χ~10), while the
             heavier neutralino (χ~20) decays into the Standard Model
             125 GeV Higgs boson and a second χ~10 are presented. The
             signal selection requires a pair of b-tagged jets consistent
             with those from a Higgs boson decay, and either an electron
             or a muon from the W boson decay, together with missing
             transverse momentum from the corresponding neutrino and the
             stable neutralinos. The analysis is based on data
             corresponding to 139 fb - 1 of s=13 TeV pp collisions
             provided by the Large Hadron Collider and recorded by the
             ATLAS detector. No statistically significant evidence of an
             excess of events above the Standard Model expectation is
             found. Limits are set on the direct production of the
             electroweakinos in simplified models, assuming pure wino
             cross-sections. Masses of χ~1±/χ~20 up to 740 GeV are
             excluded at 95% confidence level for a massless
             χ~10.},
   Doi = {10.1140/epjc/s10052-020-8050-3},
   Key = {fds351473}
}

@article{fds307637,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, M-L and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, R and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansi, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Da Costa and JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Be, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, E and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki,
             J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, JJ and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and de
             Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, QQ and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov,
             O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urban, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Armadans, RC and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, JJ and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez,
             AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi,
             G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Io, MAC and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and El
             Moursli, RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
             A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, R and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C},
   Title = {Search for direct slepton and gaugino production in final
             states with two leptons and missing transverse momentum with
             the ATLAS detector in pp collisions at √s=7
             TeV},
   Journal = {PHYSICS LETTERS B},
   Volume = {718},
   Number = {3},
   Pages = {879-901},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.11.058},
   Abstract = {A search for the electroweak pair production of charged
             sleptons and weak gauginos decaying into final states with
             two leptons is performed using 4.7 fb-1 of proton-proton
             collision data at s=7 TeV recorded with the ATLAS experiment
             at the Large Hadron Collider. No significant excesses are
             observed with respect to the prediction from Standard Model
             processes. In the scenario of direct slepton production, if
             the sleptons decay directly into the lightest neutralino,
             left-handed slepton masses between 85 and 195 GeV are
             excluded at 95% confidence level for a 20 GeV neutralino.
             Chargino masses between 110 and 340 GeV are excluded in the
             scenario of direct production of wino-like chargino pairs
             decaying into the lightest neutralino via an intermediate
             on-shell charged slepton for a 10 GeV neutralino. The
             results are also interpreted in the framework of the
             phenomenological minimal supersymmetric Standard Model. ©
             2012 CERN.},
   Doi = {10.1016/j.physletb.2012.11.058},
   Key = {fds307637}
}

@article{fds349435,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
             Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V},
   Title = {Search for direct stau production in events with two
             hadronic τ-leptons in s =13 TeV pp collisions with the
             ATLAS detector},
   Journal = {Physical Review D},
   Volume = {101},
   Number = {3},
   Year = {2020},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.101.032009},
   Abstract = {A search for the direct production of the supersymmetric
             partners of τ-leptons (staus) in final states with two
             hadronically decaying τ-leptons is presented. The analysis
             uses a dataset of pp collisions corresponding to an
             integrated luminosity of 139 fb-1, recorded with the ATLAS
             detector at the Large Hadron Collider at a center-of-mass
             energy of 13 TeV. No significant deviation from the expected
             Standard Model background is observed. Limits are derived in
             scenarios of direct production of stau pairs with each stau
             decaying into the stable lightest neutralino and one
             τ-lepton in simplified models where the two stau mass
             eigenstates are degenerate. Stau masses from 120 GeV to 390
             GeV are excluded at 95% confidence level for a massless
             lightest neutralino.},
   Doi = {10.1103/PhysRevD.101.032009},
   Key = {fds349435}
}

@article{fds307575,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou-Zeid, OS and Abramowicz, H and Abreu, H and Kuday, S and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Chekanov, S and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov, VV and Dos Santos,
             SPA and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Anulli,
             F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
   Title = {Search for direct third-generation squark pair production in
             final states with missing transverse momentum and two b-jets
             in √s = 8 TeV pp collisions with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP10(2013)189},
   Abstract = {The results of a search for pair production of
             supersymmetric partners of the Standard Model
             third-generation quarks are reported. This search uses 20.1
             fb−1 of pp collisions at √s = 8TeV collected by the
             ATLAS experiment at the Large Hadron Collider. The lightest
             bottom and top squarks (b1 and t1 respectively) are searched
             for in a final state with large missing transverse momentum
             and two jets identified as originating from b-quarks. No
             excess of events above the expected level of Standard Model
             background is found. The results are used to set upper
             limits on the visible cross section for processes beyond the
             Standard Model. Exclusion limits at the 95% confidence level
             on the masses of the third-generation squarks are derived in
             phenomenological supersymmetric R-parityconserving models in
             which either the bottom or the top squark is the lightest
             squark. The b1 is assumed to decay via b1 → bχ01 and the
             t1 via t1 → bχ±1, with undetectable products of the
             subsequent decay of the χ±1 due to the small mass
             splitting between the χ±1 and the χ01.},
   Doi = {10.1007/JHEP10(2013)189},
   Key = {fds307575}
}

@article{fds356743,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Search for direct top squark pair production in events with
             a Higgs or Z boson, and missing transverse momentum in
             √s=13 TeV pp collisions with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {8},
   Year = {2017},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2017)006},
   Abstract = {A search for direct top squark pair production resulting in
             events with either a same-flavour opposite-sign dilepton
             pair with invariant mass compatible with a Z boson or a pair
             of jets compatible with a Standard Model (SM) Higgs boson
             (h) is presented. Requirements on the missing transverse
             momentum, together with additional selections on leptons,
             jets, jets identified as originating from b-quarks are
             imposed to target the other decay products of the top squark
             pair. The analysis is performed using proton-proton
             collision data at s=13 TeV collected with the ATLAS detector
             at the LHC in 2015–2016, corresponding to an integrated
             luminosity of 36.1 fb−1. No excess is observed in the data
             with respect to the SM predictions. The results are
             interpreted in two sets of models. In the first set, direct
             production of pairs of lighter top squarks (t˜ 1) with long
             decay chains involving Z or Higgs bosons is considered. The
             second set includes direct pair production of the heavier
             top squark pairs (t˜ 2) decaying via t˜ 2→ Zt˜ 1 or t˜
             2→ ht˜ 1. The results exclude at 95% confidence level t˜
             2 and t˜ 1 masses up to about 800 GeV, extending the
             exclusion region of supersymmetric parameter space covered
             by previous LHC searches.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP08(2017)006},
   Key = {fds356743}
}

@article{fds310395,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai,
             Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Guimarães da Costa and JB and Bartoldus, R and Barton,
             AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black,
             CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm,
             J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Toro, RC and Camarda, S and Cameron, D and Caminada, LM and Armadans, RC and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Barajas, CAC and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli,
             R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi, IA and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens,
             JC},
   Title = {Search for direct top squark pair production in events with
             a [Formula: see text] boson, [Formula: see text]-jets and
             missing transverse momentum in [Formula: see text] TeV
             [Formula: see text] collisions with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {6},
   Pages = {2883},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-2883-6},
   Abstract = {A search is presented for direct top squark pair production
             using events with at least two leptons including a
             same-flavour opposite-sign pair with invariant mass
             consistent with the [Formula: see text] boson mass, jets
             tagged as originating from [Formula: see text]-quarks and
             missing transverse momentum. The analysis is performed with
             proton-proton collision data at [Formula: see text]
             collected with the ATLAS detector at the LHC in 2012
             corresponding to an integrated luminosity of
             20.3 fb[Formula: see text]. No excess beyond the Standard
             Model expectation is observed. Interpretations of the
             results are provided in models based on the direct pair
             production of the heavier top squark state ([Formula: see
             text]) followed by the decay to the lighter top squark state
             ([Formula: see text]) via [Formula: see text], and for
             [Formula: see text] pair production in natural
             gauge-mediated supersymmetry breaking scenarios where the
             neutralino ([Formula: see text]) is the next-to-lightest
             supersymmetric particle and decays producing a [Formula: see
             text] boson and a gravitino ([Formula: see text]) via the
             [Formula: see text] process.},
   Doi = {10.1140/epjc/s10052-014-2883-6},
   Key = {fds310395}
}

@article{fds307667,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, AD and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert,
             B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou,
             R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
             V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia,
             A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Begel, M and Behar Harpaz and S and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov,
             O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Search for direct top squark pair production in final states
             with one isolated lepton, jets, and missing transverse
             momentum in sqrt[s] = 7 TeV pp collisions using 4.7 fb(-10
             of ATLAS data.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {21},
   Pages = {211803},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.109.211803},
   Abstract = {A search is presented for direct top squark pair production
             in final states with one isolated electron or muon, jets,
             and missing transverse momentum in proton-proton collisions
             at sqrt[s] = 7 TeV. The measurement is based on 4.7 fb(-1)
             of data collected with the ATLAS detector at the LHC. Each
             top squark is assumed to decay to a top quark and the
             lightest supersymmetric particle (LSP). The data are found
             to be consistent with standard model expectations. Top
             squark masses between 230 GeV and 440 GeV are excluded with
             95% confidence for massless LSPs, and top squark masses
             around 400 GeV are excluded for LSP masses up to 125
             GeV.},
   Doi = {10.1103/physrevlett.109.211803},
   Key = {fds307667}
}

@article{fds348507,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and AlconadaVerzini, MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and AlvarezGonzalez, B and ÁlvarezPiqueras, D and Alviggi, MG and Amadio, BT and AmaralCoutinho, Y and Amelung, C and Amidei, D and AmorDosSantos, SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and AperioBella, L and Arabidze, G and Arai, Y and Araque, JP and AraujoFerraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
             J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic,
             M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
             C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
             AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
             NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin,
             DL and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock,
             I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt,
             BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
             S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini,
             I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
             YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
             YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Search for direct top squark pair production in final states
             with two leptons in s = 13 TeV pp collisions with the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {12},
   Pages = {898},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5445-x},
   Abstract = {The results of a search for direct pair production of top
             squarks in events with two opposite-charge leptons
             (electrons or muons) are reported, using 36.1 fb - 1 of
             integrated luminosity from proton-proton collisions at s =
             13 TeV collected by the ATLAS detector at the Large Hadron
             Collider. To cover a range of mass differences between the
             top squark t ~ and lighter supersymmetric particles, four
             possible decay modes of the top squark are targeted with
             dedicated selections: the decay t ~ → b χ ~ 1 ± into a
             <i>b</i>-quark and the lightest chargino with χ ~ 1 ± →
             W χ ~ 1 0 , the decay t ~ → t χ ~ 1 0 into an on-shell
             top quark and the lightest neutralino, the three-body decay
             t ~ → b W χ ~ 1 0 and the four-body decay t ~ → b ℓ
             ν χ ~ 1 0 . No significant excess of events is observed
             above the Standard Model background for any selection, and
             limits on top squarks are set as a function of the t ~ and
             χ ~ 1 0 masses. The results exclude at 95% confidence level
             t ~ masses up to about 720 GeV, extending the exclusion
             region of supersymmetric parameter space covered by previous
             searches.},
   Doi = {10.1140/epjc/s10052-017-5445-x},
   Key = {fds348507}
}

@article{fds347517,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
             J},
   Title = {Search for direct top squark pair production in final states
             with two tau leptons in pp collisions at [Formula:
             see text] TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {81},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-3897-z},
   Abstract = {A search for direct pair production of the supersymmetric
             partner of the top quark, decaying via a scalar tau to a
             nearly massless gravitino, has been performed using
             20 fb[Formula: see text] of proton-proton collision data at
             [Formula: see text]. The data were collected by the ATLAS
             experiment at the LHC in 2012. Top squark candidates are
             searched for in events with either two hadronically decaying
             tau leptons, one hadronically decaying tau and one light
             lepton, or two light leptons. No significant excess over the
             Standard Model expectation is found. Exclusion limits at
             [Formula: see text] confidence level are set as a function
             of the top squark and scalar tau masses. Depending on the
             scalar tau mass, ranging from the [Formula: see text] LEP
             limit to the top squark mass, lower limits between 490 and
             [Formula: see text] are placed on the top squark mass within
             the model considered.},
   Doi = {10.1140/epjc/s10052-016-3897-z},
   Key = {fds347517}
}

@article{fds310375,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Search for direct top-squark pair production in final states
             with two leptons in pp collisions at √s = 8 TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP06(2014)124},
   Abstract = {A search is presented for direct top-squark pair production
             in final states with two leptons (electrons or muons) of
             opposite charge using 20.3 fb -1 of pp collision data at
             √s = 8 TeV, collected by the ATLAS experiment at the Large
             Hadron Collider in 2012. No excess over the Standard Model
             expectation is found. The results are interpreted under the
             separate assumptions (i) that the top squark decays to a
             b-quark in addition to an on-shell chargino whose decay
             occurs via a real or virtual W boson, or (ii) that the top
             squark decays to a t-quark and the lightest neutralino. A
             top squark with a mass between 150 GeV and 445 GeV decaying
             to a b-quark and an on-shell chargino is excluded at 95%
             confidence level for a top squark mass equal to the chargino
             mass plus 10 GeV, in the case of a 1 GeV lightest
             neutralino. Top squarks with masses between 215 (90) GeV and
             530 (170) GeV decaying to an on-shell (off-shell) t-quark
             and a neutralino are excluded at 95% confidence level for a
             1 GeV neutralino. [Figure not available: see fulltext.] ©
             2014 The Author(s).},
   Doi = {10.1007/JHEP06(2014)124},
   Key = {fds310375}
}

@article{fds366278,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
             JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
             V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arguin,
             J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Austrup, VA and Avolio,
             G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey,
             AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker,
             PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian,
             R and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour,
             G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
             A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos,
             P and Basalaev, A and Basan, A and Bassalat, A and Basso, MJ and Basson,
             CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
             F and Bechtle, P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov, VA and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
             Kuutmann, E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer,
             J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia
             Bylund, O and Bethke, S and Betti, A and Bevan, AJ and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman,
             M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich,
             C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler,
             S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski,
             JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
             Bret, M and Cantero, J and Cao, Y and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carratta, G and Carter, JWS and Carter, TM and Casado,
             MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia,
             L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
             JR and Cattai, A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli,
             F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan,
             J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chau, CC and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, YS and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski,
             JJ and Cieri, D and Ciesla, KM and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
             BM and Clark, A and Clark, PJ and Clawson, SE and Clement, C and Clissa, L and Coadou, Y and Cobal, M and Coccaro, A},
   Title = {Search for Displaced Leptons in sqrt[s]=13  TeV pp
             Collisions with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {127},
   Number = {5},
   Pages = {051802},
   Year = {2021},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.127.051802},
   Abstract = {A search for charged leptons with large impact parameters
             using 139  fb^{-1} of sqrt[s]=13  TeV pp collision
             data from the ATLAS detector at the LHC is presented,
             addressing a long-standing gap in coverage of possible new
             physics signatures. Results are consistent with the
             background prediction. This search provides unique
             sensitivity to long-lived scalar supersymmetric lepton
             partners (sleptons). For lifetimes of 0.1 ns, selectron,
             smuon, and stau masses up to 720, 680, and 340  GeV,
             respectively, are excluded at 95% confidence level,
             drastically improving on the previous best limits from
             LEP.},
   Doi = {10.1103/physrevlett.127.051802},
   Key = {fds366278}
}

@article{fds310401,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Search for displaced muonic lepton jets from light Higgs
             boson decay in proton–proton collisions at √s = 7 TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {721},
   Number = {1-3},
   Pages = {32-50},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.02.058},
   Abstract = {A search is performed for collimated muon pairs displaced
             from the primary vertex produced in the decay of long-lived
             neutral particles in proton–proton collisions at s=7 TeV
             centre-of-mass energy, with the ATLAS detector at the LHC.
             In a 1.9 fb−1event sample collected during 2011, the
             observed data are consistent with the Standard Model
             background expectations. Limits on the product of the
             production cross section and the branching ratio of a Higgs
             boson decaying to hidden-sector neutral long-lived particles
             are derived as a function of the particlesʼ mean
             lifetime.},
   Doi = {10.1016/j.physletb.2013.02.058},
   Key = {fds310401}
}

@article{fds373543,
   Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk
             Cakir, I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin,
             T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben,
             M and Bouquet, R and Marchiori, G and Bhopatkar, VS and Chekanov, S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
             Gemmeren, P and Wang, R and Zhang, J and Berlendis, S and Cheu, E and Cui,
             Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Unal, M and Webb, AF and Huseynov, N and Agaras, MN and Bosman, M and Casado,
             MP},
   Title = {Search for displaced photons produced in exotic decays of
             the Higgs boson using 13 TeV pp collisions with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {108},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.108.032016},
   Abstract = {A search is performed for delayed and nonpointing photons
             originating from the displaced decay of a neutral long-lived
             particle (LLP). The analysis uses the full run 2 dataset of
             proton-proton collisions delivered by the LHC at a
             center-of-mass energy of Formula Presented between 2015 and
             2018 and recorded by the ATLAS detector, corresponding to an
             integrated luminosity of Formula Presented. The capabilities
             of the ATLAS electromagnetic calorimeter are exploited to
             precisely measure the arrival times and trajectories of
             photons. The results are interpreted in a scenario where the
             LLPs are pair produced in exotic decays of the 125 GeV Higgs
             boson, and each LLP subsequently decays into a photon and a
             particle that escapes direct detection, giving rise to
             missing transverse momentum. No significant excess is
             observed above the expectation due to Standard Model
             background processes. The results are used to set upper
             limits on the branching ratio of the exotic decay of the
             Higgs boson. A model-independent limit is also set on the
             production of photons with large values of displacement and
             time delay.},
   Doi = {10.1103/PhysRevD.108.032016},
   Key = {fds373543}
}

@article{fds307759,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for displaced vertices arising from decays of new
             heavy particles in 7 TeV pp collisions at
             ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {707},
   Number = {5},
   Pages = {478-496},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.12.057},
   Abstract = {We present the results of a search for new, heavy particles
             that decay at a significant distance from their production
             point into a final state containing charged hadrons in
             association with a high-momentum muon. The search is
             conducted in a pp-collision data sample with a
             center-of-mass energy of 7 TeV and an integrated luminosity
             of 33 pb-1 collected in 2010 by the ATLAS detector operating
             at the Large Hadron Collider. Production of such particles
             is expected in various scenarios of physics beyond the
             standard model. We observe no signal and place limits on the
             production cross-section of supersymmetric particles in an
             R-parity-violating scenario as a function of the neutralino
             lifetime. Limits are presented for different squark and
             neutralino masses, enabling extension of the limits to a
             variety of other models. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.12.057},
   Key = {fds307759}
}

@article{fds356539,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
             Pereira, R},
   Title = {Search for displaced vertices of oppositely charged leptons
             from decays of long-lived particles in pp collisions at s=13
             TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {801},
   Year = {2020},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.135114},
   Abstract = {A search for long-lived particles decaying into an
             oppositely charged lepton pair, μμ, ee, or eμ, is
             presented using 32.8fb−1 of pp collision data collected at
             s=13 TeV by the ATLAS detector at the LHC. Candidate leptons
             are required to form a vertex, within the inner tracking
             volume of ATLAS, displaced from the primary pp interaction
             region. No lepton pairs with an invariant mass greater than
             12 GeV are observed, consistent with the background
             expectations derived from data. The detection efficiencies
             for generic resonances with lifetimes (cτ) of 100–1000 mm
             decaying into a dilepton pair with masses between 0.1–1.0
             TeV are presented as a function of pT and decay radius of
             the resonances to allow the extraction of upper limits on
             the cross sections for theoretical models. The result is
             also interpreted in a supersymmetric model in which the
             lightest neutralino, produced via squark–antisquark
             production, decays into ℓ+ℓ′−ν (ℓ,ℓ′=e, μ)
             with a finite lifetime due to the presence of R-parity
             violating couplings. Cross-section limits are presented for
             specific squark and neutralino masses. For a 700 GeV squark,
             neutralinos with masses of 50–500 GeV and mean proper
             lifetimes corresponding to cτ values between 1 mm to 6 m
             are excluded. For a 1.6 TeV squark, cτ values between 3 mm
             to 1 m are excluded for 1.3 TeV neutralinos.},
   Doi = {10.1016/j.physletb.2019.135114},
   Key = {fds356539}
}

@article{fds357645,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
             JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
             V and Arcangeletti, C and Arce, ATH and Arguin, JF and Argyropoulos,
             S},
   Title = {Search for doubly and singly charged Higgs bosons decaying
             into vector bosons in multi-lepton final states with the
             ATLAS detector using proton-proton collisions at √s = 13
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {6},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2021)146},
   Abstract = {A search for charged Higgs bosons decaying into W±W± or
             W±Z bosons is performed, involving experimental signatures
             with two leptons of the same charge, or three or four
             leptons with a variety of charge combinations, missing
             transverse momentum and jets. A data sample of proton-proton
             collisions at a centre-of-mass energy of 13 TeV recorded
             with the ATLAS detector at the Large Hadron Collider between
             2015 and 2018 is used. The data correspond to a total
             integrated luminosity of 139 fb−1. The search is guided by
             a type-II seesaw model that extends the scalar sector of the
             Standard Model with a scalar triplet, leading to a
             phenomenology that includes doubly and singly charged Higgs
             bosons. Two scenarios are explored, corresponding to the
             pair production of doubly charged H±± bosons, or the
             associated production of a doubly charged H±± boson and a
             singly charged H± boson. No significant deviations from the
             Standard Model predictions are observed. H±± bosons are
             excluded at 95% confidence level up to 350 GeV and 230 GeV
             for the pair and associated production modes, respectively.
             [Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP06(2021)146},
   Key = {fds357645}
}

@article{fds308161,
   Author = {Abazov, VM and Abbott, B and Abolins, M and Acharya, BS and Adams, DL and Adams, M and Adams, T and Agelou, M and Agram, J-L and Ahmed, SN and Ahn,
             SH and Alexeev, GD and Alkhazov, G and Alton, A and Alverson, G and Alves,
             GA and Anderson, S and Andrieu, B and Arnoud, Y and Askew, A and Asman, B and Autermann, C and Avila, C and Babukhadia, L and Bacon, TC and Baden, A and Baffioni, S and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Bargassa, P and Baringer, P and Barnes, C and Barreto, J and Bartlett,
             JF and Bassler, U and Bauer, D and Bean, A and Beauceron, S and Beaudette,
             F and Begel, M and Beri, SB and Bernardi, G and Bertram, I and Besançon,
             M and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Binder, M and Bischoff, A and Black, KM and Blackler, I and Blazey, G and Blekman, F and Bloch, D and Blumenschein, U and Boehnlein, A and Bolton, TA and Bonamy, P and Borcherding, F and Borissov, G and Bos, K and Bose, T and Boswell, C and Brandt, A and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burdin, S and Burnett,
             TH and Busato, E and Butler, JM and Bystricky, J and Canelli, F and Carvalho, W and Casey, BCK and Casey, D and Cason, NM and Castilla-Valdez, H and Chakrabarti, S and Chakraborty, D and Chan,
             KM and Chandra, A and Chapin, D and Charles, F and Cheu, E and Chevalier,
             L and Cho, DK and Choi, S and Chopra, S and Christiansen, T and Christofek,
             L and Claes, D and Clark, AR and Clément, C and Coadou, Y and Colling, DJ and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Corcoran, M and Coss, J and Cothenet, A and Cousinou, M-C and Crépé-Renaudin, S and Cristetiu, M and Cummings, MAC and Cutts, D and da Motta, H and Davies,
             B and Davies, G and Davis, GA and De, K and de Jong, P and de Jong, SJ and De
             La Cruz-Burelo and E and De Oliveira Martins and C and Dean, S and Del
             Signore, K and Déliot, F and Delsart, PA and Demarteau, M and Demina,
             R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doidge, M and Dong, H and Doulas, S and Duflot, L and Dugad, SR and Duperrin, A and Dyer, J and Dyshkant, A and Eads, M and Edmunds, D and Edwards, T and Ellison, J and Elmsheuser, J and Eltzroth,
             JT and Elvira, VD and Eno, S and Ermolov, P and Eroshin, OV and Estrada, J and Evans, D and Evans, H and Evdokimov, A and Evdokimov, VN and Fast, J and Fatakia, SN and Fein, D and Feligioni, L and Ferbel, T and Fiedler, F and Filthaut, F and Fisk, HE and Fleuret, F and Fortner, M and Fox, H and Freeman, W and Fu, S and Fuess, S and Galea, CF and Gallas, E and Galyaev,
             E and Gao, M and Garcia, C and Garcia-Bellido, A and Gardner, J and Gavrilov, V and Gelé, D and Gelhaus, R and Genser, K and Gerber, CE and Gershtein, Y and Geurkov, G and Ginther, G and Goldmann, K and Golling,
             T and Gómez, B and Gounder, K and Goussiou, A and Graham, G and Grannis,
             PD and Greder, S and Green, JA and Greenlee, H and Greenwood, ZD and Gregores, EM and Grinstein, S and Grivaz, J-F and Groer, L and Grünendahl, S and Grünewald, MW and Gu, W and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Haas, A and Hadley, NJ and Haggerty,
             H and Hagopian, S and Hall, I and Hall, RE and Han, C and Han, L and Hanagaki,
             K and Hanlet, P and Harder, K and Hauptman, JM and Hauser, R and Hays, C and Hays, J and Hebert, C and Hedin, D and Heinmiller, JM and Heinson, AP and Heintz, U and Hensel, C and Hesketh, G and Hildreth, MD and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hohlfeld, M and Hong, SJ and Hooper, R and Hou, S and Hu, Y and Huang, J and Huang, Y and Iashvili, I and Illingworth,
             R and Ito, AS and Jabeen, S and Jaffré, M and Jain, S and Jain, V and Jakobs,
             K and Jenkins, A and Jesik, R and Jiang, Y and Johns, K and Johnson, M and Johnson, P and Jonckheere, A and Jonsson, P and Jöstlein, H and Juste,
             A and Kado, MM and Käfer, D and Kahl, W and Kahn, S and Kajfasz, E and Kalinin, AM and Kalk, J and Karmanov, D and Kasper, J and Kau, D and Ke, Z and Kehoe, R and Kermiche, S and Kesisoglou, S and Khanov, A and Kharchilava, A and Kharzheev, YM and Kim, KH and Klima, B and Klute, M and Kohli, JM and Kopal, M and Korablev, V and Kotcher, J and Kothari, B and Kotwal, AV and Koubarovsky, A and Kouchner, A and Kouznetsov, O and Kozelov, AV and Kozminski, J and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kurca, T and Kuznetsov, VE and Lager, S and Lahrichi, N and Landsberg, G and Lazoflores, J and Le Bihan and A-C and Lebrun, P and Lee, SW and Lee, WM and Leflat, A and Leggett, C and Lehner,
             F and Leonidopoulos, C and Lewis, P and Li, J and Li, QZ and Li, X and Lima,
             JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lobo, L and Lobodenko, A and Lokajicek, M and Lounis, A and Lu, J and Lubatti, HJ and Lucotte, A and Lueking, L and Luo, C and Lynker, M and Lyon, AL and Maciel,
             AKA and Madaras, RJ and Magnan, A-M and Maity, M and Mal, PK and Malik, S and Malyshev, VL and Manankov, V and Mao, HS and Maravin, Y and Marshall, T and Martens, M and Martin, MI and Mattingly, SEK and Mayorov, AA and McCarthy, R and McCroskey, R and McMahon, T and Meder, D and Melanson,
             HL and Melnitchouk, A and Meng, X and Merkin, M and Merritt, KW and Meyer,
             A and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mitrevski, J and Mokhov, N and Molina, J and Mondal, NK and Montgomery,
             HE and Moore, RW and Mostafa, M and Muanza, GS and Mulders, M and Mutaf,
             YD and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Naumann,
             NA and Neal, HA and Negret, JP and Nelson, S and Neustroev, P and Noeding,
             C and Nomerotski, A and Novaes, SF and Nunnemann, T and Nurse, E and O'Dell, V and O'Neil, DC and Oguri, V and Oliveira, N and Olivier, B and Oshima, N and Otero y Garzón and GJ and Padley, P and Papageorgiou, K and Parashar, N and Park, J and Park, SK and Parsons, J and Partridge, R and Parua, N and Patwa, A and Perea, PM and Perez, E and Peters, O and Pétroff, P and Petteni, M and Phaf, L and Piegaia, R and Podesta-Lerma,
             PLM and Podstavkov, VM and Pope, BG and Popkov, E and Prado da Silva,
             WL and Prosper, HB and Protopopescu, S and Przybycien, MB and Qian, J and Quadt, A and Quinn, B and Rani, KJ and Rapidis, PA and Ratoff, PN and Reay,
             NW and Renardy, J-F and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Ripp-Baudot, I and Rizatdinova, F and Royon, C and Rubinov, P and Ruchti, R and Sabirov, BM and Sajot, G and Sánchez-Hernández, A and Sanders, MP and Santoro, A and Savage, G and Sawyer, L and Scanlon, T and Schamberger, RD and Schellman, H and Schieferdecker, P and Schmitt, C and Schukin, A and Schwartzman, A and Schwienhorst, R and Sengupta, S and Shabalina, E and Shary, V and Shephard, WD and Shpakov, D and Sidwell, RA and Simak, V and Sirotenko,
             V and Skow, D and Slattery, P and Smith, RP and Smolek, K and Snow, GR and Snow, J and Snyder, S and Söldner-Rembold, S and Song, X and Song, Y and Sonnenschein, L and Sopczak, A and Sorín, V and Sosebee, M and Soustruznik, K and Souza, M and Stanton, NR and Stark, J and Steele, J and Steinbrück, G and Stevenson, K and Stolin, V and Stone, A and Stoyanova, DA and Strandberg, J and Strang, MA and Strauss, M and Ströhmer, R and Strovink, M and Stutte, L and Sznajder, A and Talby, M and Tamburello, P and Taylor, W and Telford, P and Temple, J and Tentindo-Repond, S and Thomas, E and Thooris, B and Tomoto, M and Toole,
             T},
   Title = {Search for doubly charged higgs boson pair production in the
             decay to mu(+)mu(+)mu(-)mu(-) in pp collisions at
             sqrt[s]=1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {93},
   Number = {14},
   Pages = {141801},
   Year = {2004},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.93.141801},
   Abstract = {A search for pair production of doubly charged Higgs bosons
             in the process pp -->H(++)H(--) -->mu(+)mu(+)mu(-)mu(-) is
             performed with the D0 run II detector at the Fermilab
             Tevatron. The analysis is based on a sample of inclusive
             dimuon data collected at an energy of sqrt[s]=1.96 TeV,
             corresponding to an integrated luminosity of 113 pb(-1). In
             the absence of a signal, 95% confidence level mass limits of
             M(H(+/-+/-)(L))>118.4 GeV/c(2) and M(H(+/-+/-)(R))>98.2
             GeV/c(2) are set for left-handed and right-handed doubly
             charged Higgs bosons, respectively, assuming 100% branching
             into muon pairs.},
   Doi = {10.1103/physrevlett.93.141801},
   Key = {fds308161}
}

@article{fds374254,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
             CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
             MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei,
             D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
   Title = {Search for doubly charged Higgs boson production in
             multi-lepton final states using 139 fb - 1 of
             proton–proton collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {7},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2023},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11578-9},
   Abstract = {A search for pair production of doubly charged Higgs bosons
             (H± ±), each decaying into a pair of prompt, isolated, and
             highly energetic leptons with the same electric charge, is
             presented. The search uses a proton–proton collision data
             sample at a centre-of-mass energy of 13 TeV corresponding
             to an integrated luminosity of 139 fb - 1 recorded by the
             ATLAS detector during Run 2 of the Large Hadron Collider
             (LHC). This analysis focuses on same-charge leptonic decays,
             H±±→ℓ±ℓ′± where ℓ,ℓ′=e,μ,τ , in two-,
             three-, and four-lepton channels, but only considers final
             states which include electrons or muons. No evidence of a
             signal is observed. Corresponding upper limits on the
             production cross-section of a doubly charged Higgs boson are
             derived, as a function of its mass m(H± ±) , at 95%
             confidence level. Assuming that the branching ratios to each
             of the possible leptonic final states are equal, B(H± ±→
             e±e±) = B(H± ±→ e±μ±) = B(H± ±→ μ±μ±) =
             B(H± ±→ e±τ±) = B(H± ±→ μ±τ±) = B(H± ±→
             τ±τ±) = 1 / 6 , the observed (expected) lower limit on
             the mass of a doubly charged Higgs boson is 1080 GeV
             (1065 GeV) within the left-right symmetric type-II seesaw
             model, which is the strongest limit to date produced by the
             ATLAS Collaboration. Additionally, this paper provides the
             first direct test of the Zee–Babu neutrino mass model at
             the LHC, yielding an observed (expected) lower limit of
             m(H± ±) = 900 GeV (880 GeV).},
   Doi = {10.1140/epjc/s10052-023-11578-9},
   Key = {fds374254}
}

@article{fds347473,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
             C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
             AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
             O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
             R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
             JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M},
   Title = {Search for doubly charged Higgs boson production in
             multi-lepton final states with the ATLAS detector using
             proton-proton collisions at s = 13 TeV.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {3},
   Pages = {199},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-5661-z},
   Abstract = {A search for doubly charged Higgs bosons with pairs of
             prompt, isolated, highly energetic leptons with the same
             electric charge is presented. The search uses a
             proton-proton collision data sample at a centre-of-mass
             energy of 13 TeV corresponding to 36.1 fb - 1 of integrated
             luminosity recorded in 2015 and 2016 by the ATLAS detector
             at the LHC. This analysis focuses on the decays H ± ± →
             e ± e ± , H ± ± → e ± μ ± and H ± ± → μ ± μ
             ± , fitting the dilepton mass spectra in several exclusive
             signal regions. No significant evidence of a signal is
             observed and corresponding limits on the production
             cross-section and consequently a lower limit on m ( H ± ±
             ) are derived at 95% confidence level. With ℓ ± ℓ ± =
             e ± e ± / μ ± μ ± / e ± μ ± , the observed lower
             limit on the mass of a doubly charged Higgs boson only
             coupling to left-handed leptons varies from 770 to 870 GeV
             (850 GeV expected) for B ( H ± ± → ℓ ± ℓ ± ) =
             100 % and both the expected and observed mass limits are
             above 450 GeV for B ( H ± ± → ℓ ± ℓ ± ) = 10 %
             and any combination of partial branching
             ratios.},
   Doi = {10.1140/epjc/s10052-018-5661-z},
   Key = {fds347473}
}

@article{fds308159,
   Author = {al, DAE},
   Title = {Search for Doubly Charged Higgs Bosons Decaying to Dileptons
             in pp-bar Collisions at sqrt[s]=1.96 TeV},
   Journal = {Physical Review Letters},
   Volume = {93},
   Number = {22},
   Pages = {221802},
   Year = {2004},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.93.221802},
   Abstract = {We present the results of a search for doubly charged Higgs
             bosons (H±±) decaying to dileptons (ll') using ~ 240 pb-1
             of pp-bar collision data collected by the CDF II experiment
             at the Fermilab Tevatron. In our search region, given by
             same-sign ll' mass mll'>80 GeV/c2 (100 GeV/c2 for ee
             channel), we observe no evidence for H±± production. We
             set limits on sigma (pp-bar-->H++H---- >l+l'+l-l'-) as a
             function of the mass of the H±± and the chirality of its
             couplings. Assuming exclusive same-sign dilepton decays, we
             derive lower mass limits on H±±L of 133, 136, and 115
             GeV/c2 in the ee, µµ, and eµ channels, respectively, and
             a lower mass limit of 113 GeV/c2 on H±±R in the µµ
             channel, all at the 95% confidence level.},
   Doi = {10.1103/physrevlett.93.221802},
   Key = {fds308159}
}

@article{fds307662,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
             VV and Dos Santos and SPA and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for doubly charged Higgs bosons in like-sign dilepton
             final states at √s = 7 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {12},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2244-2},
   Abstract = {A search for doubly charged Higgs bosons decaying to pairs
             of electrons and/or muons is presented. The search is
             performed using a data sample corresponding to an integrated
             luminosity of 4.7 fb−1of pp collisions at √s = 7 TeV
             collected by the ATLAS detector at the LHC. Pairs of prompt,
             isolated, high-pT leptons with the same electric charge
             (e±e±, e±μ±, μ±μ±) are selected, and their
             invariant mass distribution is searched for a narrow
             resonance. No significant excess over Standard Model
             background expectations is observed, and limits are placed
             on the cross section times branching ratio for pair
             production of doubly charged Higgs bosons. The masses of
             doubly charged Higgs bosons are constrained depending on the
             branching ratio into these leptonic final states. Assuming
             pair production, coupling to left-handed fermions, and a
             branching ratio of 100% for each final state, masses below
             409 GeV, 375 GeV, and 398 GeV are excluded for e±e±,
             e±μ±, and μ±μ±, respectively.},
   Doi = {10.1140/epjc/s10052-012-2244-2},
   Key = {fds307662}
}

@article{fds347446,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
             M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
             E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
             M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
             KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
             U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
             PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
             TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
             BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
             S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro,
             V},
   Title = {Search for doubly charged scalar bosons decaying into
             same-sign W boson pairs with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {79},
   Number = {1},
   Pages = {58},
   Year = {2019},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-6500-y},
   Abstract = {A search for doubly charged scalar bosons decaying into
             <i>W</i> boson pairs is presented. It uses a data sample
             from proton-proton collisions corresponding to an integrated
             luminosity of 36.1 fb - 1 collected by the ATLAS detector
             at the LHC at a centre-of-mass energy of 13 TeV in 2015 and
             2016. This search is guided by a model that includes an
             extension of the Higgs sector through a scalar triplet,
             leading to a rich phenomenology that includes doubly charged
             scalar bosons H ± ± . Those bosons are produced in pairs
             in proton-proton collisions and decay predominantly into
             electroweak gauge bosons H ± ± → W ± W ± .
             Experimental signatures with several leptons, missing
             transverse energy and jets are explored. No significant
             deviations from the Standard Model predictions are found.
             The parameter space of the benchmark model is excluded at
             95% confidence level for H ± ± bosons with masses between
             200 and 220 GeV.},
   Doi = {10.1140/epjc/s10052-018-6500-y},
   Key = {fds347446}
}

@article{fds30152,
   Author = {A.V. Kotwal and D. Acosta et al.},
   Title = {Search for Doubly-Charged Higgs Bosons Decaying to Dileptons
             in proton-antiproton Collisions at sqrt(s) = 1.96
             TeV},
   Journal = {Physical Review Letters},
   Volume = {93},
   Number = {221802},
   Year = {2004},
   Month = {November},
   Key = {fds30152}
}

@article{fds307692,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C},
   Title = {Search for down-type fourth generation quarks with the ATLAS
             detector in events with one lepton and hadronically decaying
             W bosons.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {3},
   Pages = {032001},
   Year = {2012},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.109.032001},
   Abstract = {This Letter presents a search for pair production of heavy
             down-type quarks decaying via b' → Wt in the lepton + jets
             channel, as b'b' → W- tW+ t → bbW+ W- W+ W- → l±
             νbbqqqqqq. In addition to requiring exactly one lepton,
             large missing transverse momentum, and at least six jets,
             the invariant mass of nearby jet pairs is used to identify
             high transverse momentum W bosons. In data corresponding to
             an integrated luminosity of 1.04  fb(-1) from pp
             collisions at sqrt[s] = 7  TeV recorded with the ATLAS
             detector, a heavy down-type quark with mass less than 480
             GeV can be excluded at the 95% confidence
             level.},
   Doi = {10.1103/physrevlett.109.032001},
   Key = {fds307692}
}

@article{fds356582,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V},
   Title = {Search for electroweak diboson production in association
             with a high-mass dijet system in semileptonic final states
             in pp collisions at s =13 TeV with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {100},
   Number = {3},
   Year = {2019},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.100.032007},
   Abstract = {This paper reports on a search for electroweak diboson
             (WW/WZ/ZZ) production in association with a high-mass dijet
             system, using data from proton-proton collisions at a
             center-of-mass energy of s=13 TeV. The data, corresponding
             to an integrated luminosity of 35.5 fb-1, were recorded with
             the ATLAS detector in 2015 and 2016 at the Large Hadron
             Collider. The search is performed in final states in which
             one boson decays leptonically, and the other boson decays
             hadronically. The hadronically decaying W/Z boson is
             reconstructed as either two small-radius jets or one
             large-radius jet using jet substructure techniques. The
             electroweak production of WW/WZ/ZZ in association with two
             jets is measured with an observed (expected) significance of
             2.7 (2.5) standard deviations, and the fiducial cross
             section is measured to be 45.1±8.6(stat.)-14.6+15.9(syst.)
             fb.},
   Doi = {10.1103/PhysRevD.100.032007},
   Key = {fds356582}
}

@article{fds356543,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob,
             M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz,
             L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA and Pereira, RA},
   Title = {Search for electroweak production of charginos and sleptons
             decaying into final states with two leptons and missing
             transverse momentum in √s=13 TeV pp collisions using the
             ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {2},
   Year = {2020},
   Month = {February},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7594-6},
   Abstract = {A search for the electroweak production of charginos and
             sleptons decaying into final states with two electrons or
             muons is presented. The analysis is based on 139 fb- 1 of
             proton–proton collisions recorded by the ATLAS detector at
             the Large Hadron Collider at s=13 TeV. Three
             R-parity-conserving scenarios where the lightest neutralino
             is the lightest supersymmetric particle are considered: the
             production of chargino pairs with decays via either W bosons
             or sleptons, and the direct production of slepton pairs. The
             analysis is optimised for the first of these scenarios, but
             the results are also interpreted in the others. No
             significant deviations from the Standard Model expectations
             are observed and limits at 95% confidence level are set on
             the masses of relevant supersymmetric particles in each of
             the scenarios. For a massless lightest neutralino, masses up
             to 420 Ge are excluded for the production of the
             lightest-chargino pairs assuming W-boson-mediated decays and
             up to 1 TeV for slepton-mediated decays, whereas for
             slepton-pair production masses up to 700 Ge are excluded
             assuming three generations of mass-degenerate
             sleptons.},
   Doi = {10.1140/epjc/s10052-019-7594-6},
   Key = {fds356543}
}

@article{fds332357,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
             JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Boos, EE and Borcherding, F and Brandt,
             A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross,
             A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV},
   Title = {Search for electroweak production of single top Quarks in
             pp̄ Collisions},
   Journal = {Physical Review D},
   Volume = {63},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2001},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.63.031101},
   Abstract = {We present a search for electroweak production of single top
             quarks in the electron+jets and muon+jets decay channels.
             The measurements use ≃ 90 pb-1 of data from Run 1 of the
             Fermilab Tevatron collider, collected at 1.8 TeV with the
             DØ detector between 1992 and 1995. We use events that
             include a tagging muon, implying the presence of a b jet, to
             set an upper limit at the 95% confidence level on the cross
             section for the s-channel process pp- → tb+X of 39 pb. The
             upper limit for the t-channel process pp- → tqb+X is 58
             pb.},
   Doi = {10.1103/PhysRevD.63.031101},
   Key = {fds332357}
}

@article{fds347484,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson,
             TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
             H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee,
             S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
             AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov,
             G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini,
             D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow,
             TM and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu,
             MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioară, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M},
   Title = {Search for electroweak production of supersymmetric
             particles in final states with two or three leptons at s =
             13 TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {12},
   Pages = {995},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-6423-7},
   Abstract = {A search for the electroweak production of charginos,
             neutralinos and sleptons decaying into final states
             involving two or three electrons or muons is presented. The
             analysis is based on 36.1 fb - 1 of s = 13  TeV
             proton-proton collisions recorded by the ATLAS detector at
             the Large Hadron Collider. Several scenarios based on
             simplified models are considered. These include the
             associated production of the next-to-lightest neutralino and
             the lightest chargino, followed by their decays into final
             states with leptons and the lightest neutralino via either
             sleptons or Standard Model gauge bosons; direct production
             of chargino pairs, which in turn decay into leptons and the
             lightest neutralino via intermediate sleptons; and slepton
             pair production, where each slepton decays directly into the
             lightest neutralino and a lepton. No significant deviations
             from the Standard Model expectation are observed and
             stringent limits at 95% confidence level are placed on the
             masses of relevant supersymmetric particles in each of these
             scenarios. For a massless lightest neutralino, masses up to
             580 GeV are excluded for the associated production of the
             next-to-lightest neutralino and the lightest chargino,
             assuming gauge-boson mediated decays, whereas for
             slepton-pair production masses up to 500 GeV are excluded
             assuming three generations of mass-degenerate
             sleptons.},
   Doi = {10.1140/epjc/s10052-018-6423-7},
   Key = {fds347484}
}

@article{fds356695,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
             M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
             JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez,
             O and Arnold, H and Arratia, M},
   Title = {Search for electroweak production of supersymmetric states
             in scenarios with compressed mass spectra at √s =13 TeV
             with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {97},
   Number = {5},
   Year = {2018},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.97.052010},
   Abstract = {A search for electroweak production of supersymmetric
             particles in scenarios with compressed mass spectra in final
             states with two low-momentum leptons and missing transverse
             momentum is presented. This search uses proton-proton
             collision data recorded by the ATLAS detector at the Large
             Hadron Collider in 2015-2016, corresponding to 36.1 fb-1 of
             integrated luminosity at s=13 TeV. Events with same-flavor
             pairs of electrons or muons with opposite electric charge
             are selected. The data are found to be consistent with the
             Standard Model prediction. Results are interpreted using
             simplified models of R-parity-conserving supersymmetry in
             which there is a small mass difference between the masses of
             the produced supersymmetric particles and the lightest
             neutralino. Exclusion limits at 95% confidence level are set
             on next-to-lightest neutralino masses of up to 145 GeV for
             Higgsino production and 175 GeV for wino production, and
             slepton masses of up to 190 GeV for pair production of
             sleptons. In the compressed mass regime, the exclusion
             limits extend down to mass splittings of 2.5 GeV for
             Higgsino production, 2 GeV for wino production, and 1 GeV
             for slepton production. The results are also interpreted in
             the context of a radiatively-driven natural supersymmetry
             model with nonuniversal Higgs boson masses.},
   Doi = {10.1103/PhysRevD.97.052010},
   Key = {fds356695}
}

@article{fds308146,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
             JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
             J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
             N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Frisch,
             H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti,
             P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
             M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher, F and Hara, K and Hare, M and Harr,
             RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays,
             C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans,
             D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato,
             Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
             SW and Lefèvre, R and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu,
             T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons,
             L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
             A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller,
             JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, AS and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager, C and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine,
             A and Rappoccio, S and Ratnikov, F and Ray, H and Reichold, A and Reisert,
             B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert,
             K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli,
             S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz,
             A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan,
             A},
   Title = {Search for electroweak single-top-quark production in pp̄
             collisions at √s = 1.96 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {1},
   Pages = {012005-1-012005-7},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.012005},
   Abstract = {We report on a search for standard model t-channel and
             s-channel single-top quark production in pp̄ collisions at
             a center of mass energy of 1.96 TeV. We use a data sample
             corresponding to 162 pb-1 recorded by the upgraded collider
             detector at Fermilab. We find no significant evidence for
             electroweak top quark production and set upper limits at the
             95% confidence level on the production cross section,
             consistent with the standard model: 10.1 pb for the
             t-channel, 13.6 pb for the s-channel and 17.8 pb for the
             combined cross section of t- and s-channel. © 2005 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.71.012005},
   Key = {fds308146}
}

@article{fds307772,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak,
             MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber,
             T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz,
             SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendel, M and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
             Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada,
             LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini,
             I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro,
             NF and Cataldi, G and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement,
             B},
   Title = {Search for events with large missing transverse momentum,
             jets, and at least two tau leptons in 7 TeV proton-proton
             collision data with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {714},
   Number = {2-5},
   Pages = {180-196},
   Publisher = {Elsevier BV},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.06.055},
   Abstract = {A search for events with large missing transverse momentum,
             jets, and at least two tau leptons has been performed using
             2 fb-1 of proton-proton collision data at s=7 TeV recorded
             with the ATLAS detector at the Large Hadron Collider. No
             excess above the Standard Model background expectation is
             observed and a 95% CL upper limit on the visible cross
             section for new phenomena is set, where the visible cross
             section is defined by the product of cross section,
             branching fraction, detector acceptance and event selection
             efficiency. A 95% CL lower limit of 32 TeV is set on the
             gauge-mediated supersymmetry breaking (GMSB) scale Λ
             independent of tanβ. These limits provide the most
             stringent tests to date in a large part of the considered
             parameter space. © 2012.},
   Doi = {10.1016/j.physletb.2012.06.055},
   Key = {fds307772}
}

@article{fds308136,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, J-F and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, W-H and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Da Ronco and S and D'Auria, S and de Barbaro, P and De Cecco and S and De Lentdecker and G and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann,
             JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
             J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
             N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, H-C and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Frisch,
             H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes,
             DW and Gerchtein, E and Giagu, S and Giannetti, P and Gibson, A and Gibson,
             K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and da Costa, JG and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
             M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
             H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Karagoz Unel and M and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and Lecompte, T and Lee, J and Lee, SW and Lefevre, R and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
             J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
             A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller,
             JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, A-S and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
             C and Pompos, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray,
             H and Reichold, A and Reisert, B and Rekovic, V and Renton, P and Rescigno,
             M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and St Denis and R and Sakumoto, WK and Salamanna,
             G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar,
             S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan, A},
   Title = {Search for excited and exotic electrons in the egamma decay
             channel in pp collisions at sqrt[s] = 1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {94},
   Number = {10},
   Pages = {101802},
   Year = {2005},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.94.101802},
   Abstract = {We present a search for excited and exotic electrons (e(*))
             decaying to an electron and a photon, both with high
             transverse momentum. We use 202 pb(-1) of data collected in
             pp collisions at sqrt[s] = 1.96 TeV with the Collider
             Detector at Fermilab II detector. No signal above standard
             model expectation is seen for associated ee(*) production.
             We discuss the e(*) sensitivity in the parameter space of
             the excited electron mass M(e(*)) and the compositeness
             energy scale Lambda. In the contact interaction model, we
             exclude 132 GeV/c(2)<M(e(*))<879 GeV/c(2) for Lambda =
             M(e(*)) at 95% confidence level (C.L.). In the
             gauge-mediated model, we exclude 126 GeV/c(2) < M(e(*)) <
             430 GeV/c(2) at 95% C.L. for the phenomenological coupling
             f/Lambda approximately 10(-2) GeV-1.},
   Doi = {10.1103/physrevlett.94.101802},
   Key = {fds308136}
}

@article{fds362579,
   Author = {Gerberich, H and Hays, C and Kotwal, A},
   Title = {Search for Excited and Exotic Muons at CDF},
   Year = {2006},
   Month = {November},
   Abstract = {We present a search for the production of excited or exotic
             muons (mu*) via the reaction pbar + p -> mu* + mu -> mu
             gamma + mu using 371/pb of data collected with the Run II
             CDF detector. In this signature-based search, we look for a
             resonance in the mu-gamma mass spectrum. The data are
             compared to standard model and detector background
             expectations, and with predictions of excited muon
             production. We use these comparisons to set limits on the
             mu* mass and compositeness scale Lambda in the contact
             interaction and gauge-mediated models.},
   Key = {fds362579}
}

@article{fds308116,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri,
             A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
             PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Ruzza, BD and Dionisi,
             C and Dittmann, JR and DiTuro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Frisch, HJ and Furic, I and Gallinaro,
             M and Galyardt, J and Garcia, JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris, N and Giolo, K and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn,
             SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr,
             RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Heijboer,
             A and Heinemann, B and Heinrich, J and Herndon, M and Hidas, D and Hill,
             CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden,
             M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon,
             EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karchin, PE and Kato, Y and Kemp, Y and Kephart,
             R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee,
             SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister,
             A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
             M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Mastrandrea, P and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
             A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Ogawa, T and Oh, SH and Oh,
             YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
             G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn,
             F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton,
             P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
             A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet,
             M},
   Title = {Search for excited and exotic muons in the μy decay channel
             in pp - collisions at s=1.96 TeV},
   Journal = {Physical Review Letters},
   Volume = {97},
   Number = {19},
   Pages = {191802},
   Year = {2006},
   ISSN = {0031-9007},
   url = {http://www.ncbi.nlm.nih.gov/pubmed/17155615},
   Abstract = {We search for excited and exotic muon states * using an
             integrated luminosity of 371pb-1 of pp collision data at
             s=1.96TeV. We search for associated production of * followed
             by the decay *. We compare the data to model predictions as
             a function of the mass of the excited muon M *, the
             compositeness energy scale , and the gauge coupling factor
             f. No signal above the standard model expectation is
             observed. We exclude 107&lt;M *&lt;853GeV/c2 for =M * in the
             contact interaction model, and 100&lt;M *&lt;410GeV/c2 for
             f/=10-2GeV-1 in the gauge-mediated model, both at the 95%
             confidence level. © 2006 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.97.191802},
   Key = {fds308116}
}

@article{fds307581,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {Search for excited electrons and muons in √s=8 TeV
             proton-proton collisions with the ATLAS detector},
   Journal = {New Journal of Physics},
   Volume = {15},
   Number = {9},
   Pages = {093011-093011},
   Publisher = {IOP Publishing},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1088/1367-2630/15/9/093011},
   Abstract = {The ATLAS detector at the Large Hadron Collider is used to
             search for excited electrons and excited muons in the
             channel pp → ℓℓ* → ℓℓγ, assuming that excited
             leptons are produced via contact interactions. The analysis
             is based on 13 fb-1 of pp collisions at a centre-of-mass
             energy of 8 TeV. No evidence for excited leptons is found,
             and a limit is set at the 95% credibility level on the cross
             section times branching ratio as a function of the
             excited-lepton mass mℓ*. For mℓ* 0.8 TeV, the respective
             upper limits on σB(ℓ* → ℓγ) are 0.75 and 0.90 fb for
             the e* and μ* searches. Limits on σB are converted into
             lower bounds on the compositeness scale Λ. In the special
             case where Λ = m ℓ*, excited-electron and excited-muon
             masses below 2.2 TeV are excluded. © CERN
             2013.},
   Doi = {10.1088/1367-2630/15/9/093011},
   Key = {fds307581}
}

@article{fds356580,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA and Pereira, RA and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arling,
             JH},
   Title = {Search for excited electrons singly produced in
             proton–proton collisions at √s=13Te with the ATLAS
             experiment at the LHC},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {9},
   Year = {2019},
   Month = {September},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7295-1},
   Abstract = {A search for excited electrons produced in pp collisions at
             s = 13 Te via a contact interaction qq¯ → ee∗ is
             presented. The search uses 36.1 fb- 1 of data collected in
             2015 and 2016 by the ATLAS experiment at the Large Hadron
             Collider. Decays of the excited electron into an electron
             and a pair of quarks (eqq¯) are targeted in final states
             with two electrons and two hadronic jets, and decays via a
             gauge interaction into a neutrino and a W boson (νW) are
             probed in final states with an electron, missing transverse
             momentum, and a large-radius jet consistent with a
             hadronically decaying W boson. No significant excess is
             observed over the expected backgrounds. Upper limits are
             calculated for the pp→ ee∗→ eeqq¯ and pp→ ee∗→
             eνW production cross sections as a function of the excited
             electron mass me∗ at 95% confidence level. The limits are
             translated into lower bounds on the compositeness scale
             parameter Λ of the model as a function of me∗. For
             me∗<0.5 Te, the lower bound for Λ is 11 Te. In the
             special case of me∗=Λ, the values of me∗<4.8 Te are
             excluded. The presented limits on Λ are more stringent than
             those obtained in previous searches.},
   Doi = {10.1140/epjc/s10052-019-7295-1},
   Key = {fds356580}
}

@article{fds307735,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for excited leptons in proton-proton collisions at
             √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.072003},
   Abstract = {The ATLAS detector is used to search for excited leptons in
             the electromagnetic radiative decay channel *→γ. Results
             are presented based on the analysis of pp collisions at a
             center-of-mass energy of 7 TeV corresponding to an
             integrated luminosity of 2.05fb-1. No evidence for excited
             leptons is found, and limits are set on the compositeness
             scale Λ as a function of the excited lepton mass m *. In
             the special case where Λ=m *, excited electron and muon
             masses below 1.87 TeV and 1.75 TeV are excluded at 95% C.L.,
             respectively. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.85.072003},
   Key = {fds307735}
}

@article{fds308047,
   Author = {Aaltonen, T and Abulencia, A and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev,
             K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Behari,
             S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carrillo, S and Carlsmith, D and Caron, B and Carosi, R and Carron,
             S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Daronco, S and Datta, M and D'Auria, S and Davies, T and Dagenhart, D and de Barbaro, P and De
             Cecco, S and Deisher, A and De Lentdecker and G and De Lorenzo and G and Dell'orso, M and Delli Paoli and F and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Dörr,
             C and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron,
             J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
             M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro,
             M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani,
             M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
             da Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
             RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson,
             C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl,
             D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel,
             U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraan, AC and Kraus,
             J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
             C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
             J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli, F and Marginean,
             R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty,
             R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel,
             P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles,
             J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher,
             G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moon, CS and Moore,
             R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee,
             A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
             G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pinfold, J and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
             R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov,
             A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar,
             S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
             A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet,
             M},
   Title = {Search for exclusive gammagamma production in Hadron-Hadron
             collisions.},
   Journal = {Physical review letters},
   Volume = {99},
   Number = {24},
   Pages = {242002},
   Year = {2007},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.99.242002},
   Abstract = {We have searched for exclusive gammagamma production in
             proton-antiproton collisions at sqrt[s]=1.96 TeV, using 532
             pb(-1) of integrated luminosity taken by the run II Collider
             Detector at Fermilab. The event signature requires two
             electromagnetic showers, each with transverse energy E(T)>5
             GeV and pseudorapidity |eta|<1.0, with no other particles
             detected in the event. Three candidate events are observed.
             We discuss the consistency of the three events with
             gammagamma, pi(0)pi(0), or eta eta production. The
             probability that other processes fluctuate to >or=3 events
             is 1.7x10(-4). An upper limit on the cross section of pp-->p
             + gammagamma + p production is set at 410 fb with 95%
             confidence level.},
   Doi = {10.1103/physrevlett.99.242002},
   Key = {fds308047}
}

@article{fds356675,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for exclusive Higgs and Z boson decays to ϕγ and
             ργ with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {7},
   Year = {2018},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2018)127},
   Abstract = {A search for the exclusive decays of the Higgs and Z bosons
             to a ϕ or ρ meson and a photon is performed with a pp
             collision data sample corresponding to an integrated
             luminosity of up to 35.6 fb−1 collected at s=13 TeV with
             the ATLAS detector at the CERN Large Hadron Collider. These
             decays have been suggested as a probe of the Higgs boson
             couplings to light quarks. No significant excess of events
             is observed above the background, as expected from the
             Standard Model. Upper limits at 95% confidence level were
             obtained on the branching fractions of the Higgs boson
             decays to ϕγ and ργ of 4.8 × 10−4 and 8.8 × 10−4,
             respectively. The corresponding 95% confidence level upper
             limits for the Z boson decays are 0.9 × 10−6 and 25 ×
             10−6 for ϕγ and ργ, respectively.[Figure not
             available: see fulltext.].},
   Doi = {10.1007/JHEP07(2018)127},
   Key = {fds356675}
}

@article{fds375876,
   Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
             M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
             PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
             Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
             V and Arcangeletti, C and Arce, ATH and Arena, E},
   Title = {Search for exclusive Higgs and Z boson decays to ωγ and
             Higgs boson decays to Kγ with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {847},
   Year = {2023},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.138292},
   Abstract = {Searches for the exclusive decays of the Higgs boson to an
             ω meson and a photon or a K⁎ meson and a photon can probe
             flavour-conserving and flavour-violating Higgs boson
             couplings to light quarks, respectively. Searches for these
             decays, along with the analogous Z boson decay to an ω
             meson and a photon, are performed with a pp collision data
             sample corresponding to integrated luminosities of up to 134
             fb−1 collected at s=13 TeV with the ATLAS detector at the
             CERN Large Hadron Collider. The obtained 95%
             confidence-level upper limits on the respective branching
             fractions are B(H→ωγ)<5.5×10−4, B(H→K⁎γ)<2.2×10−4
             and B(Z→ωγ)<3.9×10−6. The limits for H→ωγ and
             Z→ωγ are 370 times and 140 times the Standard Model
             expected values, respectively. The result for Z→ωγ
             corresponds to a two-orders-of-magnitude improvement over
             the limit obtained by the DELPHI experiment at
             LEP.},
   Doi = {10.1016/j.physletb.2023.138292},
   Key = {fds375876}
}

@article{fds307975,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi,
             F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley,
             M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell,
             M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
             S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Di Canto and A and di Giovanni, GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Garosi, P and Genser, K and Gerberich,
             H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
             da Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas,
             D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
             JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko,
             S and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee,
             SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Pagan Griso and S and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pinera, L and Pinfold, J and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
             J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Rutherford, B and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel,
             S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sinervo,
             P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M},
   Title = {Search for exclusive Z-boson production and observation of
             high-mass pp[over ]-->pgammagammap[over ]-->pl;{+}l;{-}p[over
             ] events in pp[over ] collisions at sqrt[s]=1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {22},
   Pages = {222002},
   Year = {2009},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.102.222002},
   Abstract = {This Letter presents a search for exclusive Z boson
             production in proton-antiproton collisions at sqrt[s]=1.96
             TeV, using the CDF II detector. No exclusive Z-->l;{+}l;{-}
             candidates are observed and the first upper limit on the
             exclusive Z cross section in hadron collisions is found to
             be sigma_{excl}(Z)<0.96 pb at 95% confidence level. In
             addition, eight candidate exclusive dilepton events from the
             process pp[over ]-->pgammagammap[over ]-->pl;{+}l;{-}p[over
             ] are observed, and a measurement of the cross section for
             M_{ll}>40 GeV/c;{2} and |eta_{l}|<4 is found to be
             sigma=0.24_{-0.10};{+0.13} pb, which is consistent with the
             standard model prediction.},
   Doi = {10.1103/physrevlett.102.222002},
   Key = {fds307975}
}

@article{fds308071,
   Author = {Abulencia, and A, and others},
   Title = {Search for Exotic $S=-2$ Baryons in $p\bar{p}$ Collisions at
             $\sqrt{s}=1.96\,TeV$},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {3},
   Pages = {032003},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.032003},
   Abstract = {A search for a manifestly exotic S=-2 baryon state decaying
             to Xi-pi-, and its neutral partner decaying to Xi-pi+, has
             been performed using 220 pb-1 of p[overline p] collisions at
             sqrt(s)=1.96 TeV collected by the Collider Detector at
             Fermilab. The Xi- trajectories were measured in a silicon
             tracker before their decay, resulting in a sample with low
             background and excellent position resolution. No evidence
             was found for S=-2 pentaquark candidates in the invariant
             mass range of 1600--2100 MeV/c2. Upper limits on the product
             of pentaquark production cross section times its branching
             fraction to Xi-pi+,-, relative to the cross section of the
             well-established Xi(1530) resonance, are presented for
             neutral and doubly negative candidates with pT>2 GeV/c and
             |y|},
   Doi = {10.1103/PhysRevD.75.032003},
   Key = {fds308071}
}

@article{fds361805,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala,
             J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada
             Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
             M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF},
   Title = {Search for exotic decays of the Higgs boson into b b¯ and
             missing transverse momentum in pp collisions at √s = 13
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2022},
   Number = {1},
   Year = {2022},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2022)063},
   Abstract = {A search for the exotic decay of the Higgs boson (H) into a
             bb¯ resonance plus missing transverse momentum is
             described. The search is performed with the ATLAS detector
             at the Large Hadron Collider using 139 fb−1 of pp
             collisions at s = 13 TeV. The search targets events from ZH
             production in an NMSSM scenario where H → χ~20χ~10, with
             χ~20→aχ~10, where a is a light pseudoscalar Higgs boson
             and χ~1,20 are the two lightest neutralinos. The decay of
             the a boson into a pair of b-quarks results in a peak in the
             dijet invariant mass distribution. The final-state signature
             consists of two leptons, two or more jets, at least one of
             which is identified as originating from a b-quark, and
             missing transverse momentum. Observations are consistent
             with Standard Model expectations and upper limits are set on
             the product of cross section times branching ratio for a
             three-dimensional scan of the masses of the χ~20, χ~10 and
             a boson. [Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP01(2022)063},
   Key = {fds361805}
}

@article{fds360769,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S and Arling, JH},
   Title = {Search for exotic decays of the Higgs boson into long-lived
             particles in pp collisions at √s = 13 TeV using displaced
             vertices in the ATLAS inner detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {11},
   Year = {2021},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2021)229},
   Abstract = {A novel search for exotic decays of the Higgs boson into
             pairs of long-lived neutral particles, each decaying into a
             bottom quark pair, is performed using 139 fb−1 of s = 13
             TeV proton-proton collision data collected with the ATLAS
             detector at the LHC. Events consistent with the production
             of a Higgs boson in association with a leptonically decaying
             Z boson are analysed. Long-lived particle (LLP) decays are
             reconstructed from inner-detector tracks as displaced
             vertices with high mass and track multiplicity relative to
             Standard Model processes. The analysis selection requires
             the presence of at least two displaced vertices, effectively
             suppressing Standard Model backgrounds. The residual
             background contribution is estimated using a data-driven
             technique. No excess over Standard Model predictions is
             observed, and upper limits are set on the branching ratio of
             the Higgs boson to LLPs. Branching ratios above 10% are
             excluded at 95% confidence level for LLP mean proper
             lifetimes cτ as small as 4 mm and as large as 100 mm. For
             LLP masses below 40 GeV, these results represent the most
             stringent constraint in this lifetime regime. [Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP11(2021)229},
   Key = {fds360769}
}

@article{fds307606,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Search for extra dimensions in diphoton events from
             proton-proton collisions at √s= 7 TeV in the ATLAS
             detector at the LHC},
   Journal = {New Journal of Physics},
   Volume = {15},
   Number = {4},
   Pages = {043007-043007},
   Publisher = {IOP Publishing},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1088/1367-2630/15/4/043007},
   Abstract = {The large difference between the Planck scale and the
             electroweak scale, known as the hierarchy problem, is
             addressed in certain models through the postulate of extra
             spatial dimensions. A search for evidence of extra spatial
             dimensions in the diphoton channel has been performed using
             the full set of proton-proton collisions at √s = 7 TeV
             recorded in 2011 with the ATLAS detector at the CERN Large
             Hadron Collider. This dataset corresponds to an integrated
             luminosity of 4.9 fb1. The diphoton invariant mass spectrum
             is observed to be in good agreement with the Standard Model
             expectation. In the context of the model proposed by
             Arkani-Hamed, Dimopoulos and Dvali, 95% confidence level
             lower limits of between 2.52 and 3.92 TeV are set on the
             ultraviolet cutoff scale MS depending on the number of extra
             dimensions and the theoretical formalism used. In the
             context of the Randall-Sundrum model, a lower limit of 2.06
             (1.00) TeV at 95% confidence level is set on the mass of the
             lightest graviton for couplings of k/MPl = 0.1(0.01).
             Combining with the ATLAS dilepton searches based on the 2011
             data, the 95% confidence level lower limit on the
             Randall-Sundrum graviton mass is further tightened to 2.23
             (1.03) TeV for k/ MPl= 0.1(0.01).© CERN 2013 for the
             benefit of the ATLAS Collaboration.},
   Doi = {10.1088/1367-2630/15/4/043007},
   Key = {fds307606}
}

@article{fds307732,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov,
             A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
             JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez,
             VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B},
   Title = {Search for extra dimensions using diphoton events in 7 TeV
             proton-proton collisions with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {710},
   Number = {4-5},
   Pages = {538-556},
   Publisher = {Elsevier BV},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.03.022},
   Abstract = {Using data recorded in 2011 with the ATLAS detector at the
             Large Hadron Collider, a search for evidence of extra
             spatial dimensions has been performed through an analysis of
             the diphoton final state. The analysis uses data
             corresponding to an integrated luminosity of 2.12fb-1 of
             s=7TeV proton-proton collisions. The diphoton invariant mass
             (mγγ) spectrum is observed to be in good agreement with
             the expected Standard Model background. In the large extra
             dimension scenario of Arkani-Hamed, Dimopoulos and Dvali,
             the results provide 95% CL lower limits on the fundamental
             Planck scale between 2.27 and 3.53 TeV, depending on the
             number of extra dimensions and the theoretical formalism
             used. The results also set 95% CL lower limits on the
             lightest Randall-Sundrum graviton mass of between 0.79 and
             1.85 TeV, for values of the dimensionless coupling k/-1 Pl
             varying from 0.01 to 0.1. Combining with previously
             published ATLAS results from the dielectron and dimuon final
             states, the 95% CL lower limit on the Randall-Sundrum
             graviton mass for k/M-1Pl=0.01 (0.1) is 0.80 (1.95) TeV. ©
             2012 CERN.},
   Doi = {10.1016/j.physletb.2012.03.022},
   Key = {fds307732}
}

@article{fds307727,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for FCNC single top-quark production at √s=7 TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {712},
   Number = {4-5},
   Pages = {351-369},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {June},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.05.022},
   Abstract = {A search for the production of single top-quarks via
             flavour-changing neutral-currents is presented. Data
             collected with the ATLAS detector at a centre-of-mass energy
             of s=7 TeV, corresponding to an integrated luminosity of
             2.05 fb−1, are used. Candidate events with a semileptonic
             top-quark decay signature are classified as signal- or
             background-like events by using several kinematic variables
             as input to a neural network. No signal is observed in the
             neural network output distribution and a Bayesian upper
             limit is placed on the production cross-section. The
             observed upper limit at 95% confidence level on the
             cross-section multiplied by the t→Wb branching fraction is
             measured to be σqg→t×B(t→Wb)<3.9 pb. This upper limit
             is converted using a model-independent approach into upper
             limits on the coupling strengths κugt/Λ<6.9⋅10−3
             TeV−1 and κcgt/Λ<1.6⋅10−2 TeV−1, where Λ is the
             new physics scale, and on the branching fractions
             B(t→ug)<5.7⋅10−5 and B(t→cg)<2.7⋅10−4.},
   Doi = {10.1016/j.physletb.2012.05.022},
   Key = {fds307727}
}

@booklet{Abbott98l,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
             EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis,
             E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram,
             I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {Search for first generation scalar leptoquark pairs in pp
             collisions at √ s = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {10},
   Pages = {2051-2056},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.2051},
   Abstract = {We have searched for first generation scalar leptoquark (LQ)
             pairs in the ev + jets channel using pp collider data (∫L
             dt ≈ 115pb-1) collected by the D0 experiment at the
             Fermilab Tevatron during 1992-1996. The analysis yields no
             candidate events. We combine the results with those from the
             ee + jets vv + jets channels to obtain 95% confidence level
             (C.L.) upper limits on the LQ pair production cross section
             as a function of mass and of β, the branching fraction to a
             charged lepton. Comparing with the next-to-leading order
             theory, we set 95% C.L. lower limits on the LQ mass of 225,
             204, and 79 GeV/c2 for β = 1, 1/2, and 0, respectively. ©
             1998 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.80.2051},
   Key = {Abbott98l}
}

@article{fds307734,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov,
             A},
   Title = {Search for first generation scalar leptoquarks in pp
             collisions at s=7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {709},
   Number = {3},
   Pages = {158-176},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.004},
   Abstract = {We report a search for first generation scalar leptoquarks
             using 1.03fb-1 of proton-proton collisions data produced by
             the Large Hadron Collider at s=7 TeV and recorded by the
             ATLAS experiment. Leptoquarks are sought via their decay
             into an electron or neutrino and a quark, producing events
             with two oppositely charged electrons and at least two jets,
             or events with an electron, missing transverse momentum and
             at least two jets. Control data samples are used to validate
             background predictions from Monte Carlo simulation. In the
             signal region, the observed event yields are consistent with
             the background expectations. We exclude at 95% confidence
             level the production of first generation scalar leptoquark
             with masses mLQ<660(607) GeV when assuming the branching
             fraction of a leptoquark to a charged lepton is equal to 1.0
             (0.5). © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.02.004},
   Key = {fds307734}
}

@article{fds308186,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin,
             B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto,
             J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
             F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and Jong, SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot,
             L},
   Title = {Search for first-generation scalar and vector
             leptoquarks},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {64},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2001},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.64.092004},
   Abstract = {We describe a search for the pair production of
             first-generation scalar and vector leptoquarks in the
             [Formula Presented] and [Formula Presented] channels by the
             DØ Collaboration. The data are from the 1992–1996
             [Formula Presented] run at [Formula Presented] at the
             Fermilab Tevatron collider. We find no evidence for
             leptoquark production; in addition, no kinematically
             interesting events are observed using relaxed selection
             criteria. The results from the [Formula Presented] and
             [Formula Presented] channels are combined with those from a
             previous DØ analysis of the [Formula Presented] channel to
             obtain 95% confidence level (C.L.) upper limits on the
             leptoquark pair-production cross section as a function of
             mass and of [Formula Presented] the branching fraction to a
             charged lepton. These limits are compared to
             next-to-leading-order theory to set 95% C.L. lower limits on
             the mass of a first-generation scalar leptoquark of 225,
             204, and 79 [Formula Presented] for [Formula Presented]
             [Formula Presented] and 0, respectively. For vector
             leptoquarks with gauge (Yang-Mills) couplings, 95% C.L.
             lower limits of 345, 337, and 206 [Formula Presented] are
             set on the mass for [Formula Presented] [Formula Presented]
             and 0, respectively. Mass limits for vector leptoquarks are
             also set for anomalous vector couplings. © 2001 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.64.092004},
   Key = {fds308186}
}

@article{fds308115,
   Author = {Acosta, and D, and others},
   Title = {Search for first-generation scalar leptoquarks in pp-bar
             collisions at sqrt[s]=1.96 TeV},
   Journal = {Phys. Rev.},
   Volume = {D72},
   Number = {5},
   Pages = {051107},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.051102},
   Abstract = {Results on a search for pair production of second-generation
             scalar leptoquark in pp̄ collisions at s=1.96TeV are
             reported. The data analyzed were collected by the CDF
             detector during the 2002-2003 Tevatron Run II and correspond
             to an integrated luminosity of 198pb-1. Leptoquarks (LQ) are
             sought through their decay into (charged) leptons and
             quarks, with final state signatures represented by two muons
             and jets and one muon, large transverse missing energy and
             jets. We observe no evidence for LQ production and derive
             95% C.L. upper limits on the LQ production cross sections as
             well as lower limits on their mass as a function of β,
             where β is the branching fraction for LQ→μq. © 2006 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.73.051102},
   Key = {fds308115}
}

@article{fds356668,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A},
   Title = {Search for flavor-changing neutral currents in top quark
             decays t →Hc and t →Hu in multilepton final states in
             proton-proton collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {3},
   Year = {2018},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.032002},
   Abstract = {Flavor-changing neutral currents are not present in the
             Standard Model at tree level and are suppressed in loop
             processes by the unitarity of the Cabibbo-Kobayashi-Maskawa
             matrix; the corresponding rates for top quark decay
             processes are experimentally unobservable. Extensions of the
             Standard Model can generate new flavor-changing neutral
             current processes, leading to signals which, if observed,
             would be unambiguous evidence of new interactions. A data
             set corresponding to an integrated luminosity of 36.1 fb-1
             of pp collisions at a center-of-mass energy of s=13 TeV
             recorded with the ATLAS detector at the Large Hadron
             Collider is used to search for top quarks decaying to up or
             charm quarks with the emission of a Higgs boson, with
             subsequent Higgs boson decay to final states with at least
             one electron or muon. No signal is observed and limits on
             the branching fractions B(t→Hc)<0.16% and B(t→Hu)<0.19%
             at 95% confidence level are obtained (with expected limits
             of 0.15% in both cases).},
   Doi = {10.1103/PhysRevD.98.032002},
   Key = {fds356668}
}

@article{fds373910,
   Author = {Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Sharma, AS and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk
             Cakir, I and Sultansoy, S and Adam Bourdarios and C and Belfkir, M and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Franco,
             L and Goy, C and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Lafaye, R and Levêque, J and Lorenzo Martinez and N and Portales, L and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem,
             L and Wingerter-Seez, I and Abulaiti, Y and Bhopatkar, VS and Chekanov,
             S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love,
             J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
             Gemmeren, P and Zhang, J and Berlendis, S and Cheu, E and Cui, Z and Delitzsch, CM and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Little, JD and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas,
             L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Gazis, EN and Gkountoumis, P and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Zacharis, G and Andeen, T and Burton, CD and Choi, K and Nikiforou, N and Onyisi, PUE and Panchal, DK and Roy, A and Unal, M and Webb, AF and Adiguzel,
             A},
   Title = {Search for flavor-changing neutral-current couplings between
             the top quark and the Z boson with proton-proton
             collisions at √s=13  TeV with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {108},
   Number = {3},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.108.032019},
   Abstract = {A search for flavor-changing neutral-current couplings
             between a top quark, an up or charm quark, and a Formula
             Presented boson is presented, using proton-proton collision
             data at Formula Presented collected by the ATLAS detector at
             the Large Hadron Collider. The analyzed data set corresponds
             to an integrated luminosity of Formula Presented. The search
             targets both single-top-quark events produced as Formula
             Presented (with Formula Presented, Formula Presented) and
             top-quark-pair events, with one top quark decaying through
             the Formula Presented channel. The analysis considers events
             with three leptons (electrons or muons), a Formula
             Presented-tagged jet, possible additional jets, and missing
             transverse momentum. The data are found to be consistent
             with the background-only hypothesis and 95% confidence-level
             limits on the Formula Presented branching ratios, assuming
             only tensor operators of the Standard Model effective field
             theory framework contribute to the Formula Presented
             vertices. These are Formula Presented (Formula Presented)
             for Formula Presented (Formula Presented) for a left-handed
             Formula Presented coupling, and Formula Presented (Formula
             Presented) in the case of a right-handed coupling. These
             results are interpreted as 95% CL upper limits on the
             strength of the corresponding couplings, yielding limits for
             Formula Presented and Formula Presented (Formula Presented
             and Formula Presented) of 0.15 (0.16), and limits for
             Formula Presented and Formula Presented (Formula Presented
             and Formula Presented) of 0.22 (0.21), assuming a
             new-physics energy scale Formula Presented of 1
             TeV.},
   Doi = {10.1103/PhysRevD.108.032019},
   Key = {fds373910}
}

@article{fds313611,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for flavour-changing neutral current top quark decays
             t → Hq in pp collisions at √s=8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {12},
   Pages = {1-65},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2015)061},
   Abstract = {Abstract: A search for flavour-changing neutral current
             decays of a top quark to an uptype quark (q = u, c) and the
             Standard Model Higgs boson, where the Higgs boson decays
             to(Formula Presented.), is presented. The analysis searches
             for top quark pair events in which one top quark decays to
             Wb, with the W boson decaying leptonically, and the other
             top quark decays to Hq. The search is based on pp collisions
             at (Formula Presented.) TeV recorded in 2012 with the ATLAS
             detector at the CERN Large Hadron Collider and uses an
             integrated luminosity of 20.3 fb−1. Data are analysed in
             the lepton-plus-jets final state, characterised by an
             isolated electron or muon and at least four jets. The search
             exploits the high multiplicity of b-quark jets
             characteristic of signal events, and employs a likelihood
             discriminant that uses the kinematic differences between the
             signal and the background, which is dominated by (Formula
             Presented.) decays. No significant excess of events above
             the background expectation is found, and observed (expected)
             95% CL upper limits of 0.56% (0.42%) and 0.61% (0.64%) are
             derived for the t → Hc and t → Hu branching ratios
             respectively. The combination of this search with other
             ATLAS searches in the H → γγ and H → WW*, ττ decay
             modes significantly improves the sensitivity, yielding
             observed (expected) 95% CL upper limits on the t → Hc and
             t → Hu branching ratios of 0.46% (0.25%) and 0.45% (0.29%)
             respectively. The corresponding combined observed (expected)
             upper limits on the |λtcH| and |λtuH| couplings are 0.13
             (0.10) and 0.13 (0.10) respectively. These are the most
             restrictive direct bounds on tqH interactions measured so
             far.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP12(2015)061},
   Key = {fds313611}
}

@article{fds356676,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada
             Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
             M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for flavour-changing neutral current top-quark decays
             t → qZ in proton-proton collisions at √s=13 TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {7},
   Year = {2018},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2018)176},
   Abstract = {A search for flavour-changing neutral-current processes in
             top-quark decays is presented. Data collected with the ATLAS
             detector from proton-proton collisions at the Large Hadron
             Collider at a centre-of-mass energy of s=13 TeV,
             corresponding to an integrated luminosity of 36.1 fb−1,
             are analysed. The search is performed using top-quark pair
             events, with one top quark decaying through the t → qZ (q
             = u, c) flavour-changing neutral-current channel, and the
             other through the dominant Standard Model mode t → bW.
             Only Z boson decays into charged leptons and leptonic W
             boson decays are considered as signal. Consequently, the
             final-state topology is characterized by the presence of
             three isolated charged leptons (electrons or muons), at
             least two jets, one of the jets originating from a b-quark,
             and missing transverse momentum from the undetected
             neutrino. The data are consistent with Standard Model
             background contributions, and at 95% confidence level the
             search sets observed (expected) upper limits of 1.7 ×
             10−4 (2.4 × 10−4) on the t → uZ branching ratio and
             2.4 × 10−4 (3.2 × 10−4) on the t → cZ branching
             ratio, constituting the most stringent limits to
             date.[Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP07(2018)176},
   Key = {fds356676}
}

@article{fds347516,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T},
   Title = {Search for flavour-changing neutral current top-quark decays
             to [Formula: see text] in [Formula: see text] collision data
             collected with the ATLAS detector at [Formula: see
             text] TeV.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {12},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3851-5},
   Abstract = {A search for the flavour-changing neutral-current decay
             [Formula: see text] is presented. Data collected by the
             ATLAS detector during 2012 from proton-proton collisions at
             the Large Hadron Collider at a centre-of-mass energy of
             [Formula: see text] TeV, corresponding to an integrated
             luminosity of 20.3 fb[Formula: see text], are analysed.
             Top-quark pair-production events with one top quark decaying
             through the [Formula: see text] ([Formula: see text])
             channel and the other through the dominant Standard Model
             mode [Formula: see text] are considered as signal. Only the
             decays of the <i>Z</i> boson to charged leptons and leptonic
             <i>W</i> boson decays are used. No evidence for a signal is
             found and an observed (expected) upper limit on the
             [Formula: see text] branching ratio of [Formula: see text]
             ([Formula: see text]) is set at the 95 % confidence
             level.},
   Doi = {10.1140/epjc/s10052-015-3851-5},
   Key = {fds347516}
}

@article{fds356545,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
             Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V},
   Title = {Search for flavour-changing neutral currents in processes
             with one top quark and a photon using 81 fb−1
             of pp collisions at s=13TeV with the ATLAS
             experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {800},
   Year = {2020},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.135082},
   Abstract = {A search for flavour-changing neutral current (FCNC) events
             via the coupling of a top quark, a photon, and an up or
             charm quark is presented using 81 fb−1 of proton–proton
             collision data taken at a centre-of-mass energy of 13 TeV
             with the ATLAS detector at the LHC. Events with a photon, an
             electron or muon, a b-tagged jet, and missing transverse
             momentum are selected. A neural network based on kinematic
             variables differentiates between events from signal and
             background processes. The data are consistent with the
             background-only hypothesis, and limits are set on the
             strength of the tqγ coupling in an effective field theory.
             These are also interpreted as 95% CL upper limits on the
             cross section for FCNC tγ production via a left-handed
             (right-handed) tuγ coupling of 36 fb (78 fb) and on the
             branching ratio for t→γu of 2.8×10−5 (6.1×10−5). In
             addition, they are interpreted as 95% CL upper limits on the
             cross section for FCNC tγ production via a left-handed
             (right-handed) tcγ coupling of 40 fb (33 fb) and on the
             branching ratio for t→γc of 22×10−5
             (18×10−5).},
   Doi = {10.1016/j.physletb.2019.135082},
   Key = {fds356545}
}

@article{fds372127,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
             L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
             JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
             JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
             VA},
   Title = {Search for flavour-changing neutral-current couplings
             between the top quark and the photon with the ATLAS detector
             at s=13 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {842},
   Year = {2023},
   Month = {July},
   url = {http://dx.doi.org/10.1016/j.physletb.2022.137379},
   Abstract = {This letter documents a search for flavour-changing neutral
             currents (FCNCs), which are strongly suppressed in the
             Standard Model, in events with a photon and a top quark with
             the ATLAS detector. The analysis uses data collected in pp
             collisions at s=13 TeV during Run 2 of the LHC,
             corresponding to an integrated luminosity of 139 fb−1.
             Both FCNC top-quark production and decay are considered. The
             final state consists of a charged lepton, missing transverse
             momentum, a b-tagged jet, one high-momentum photon and
             possibly additional jets. A multiclass deep neural network
             is used to classify events either as signal in one of the
             two categories, FCNC production or decay, or as background.
             No significant excess of events over the background
             prediction is observed and 95% CL upper limits are placed on
             the strength of left- and right-handed FCNC interactions.
             The 95% CL bounds on the branching fractions for the FCNC
             top-quark decays, estimated (expected) from both top-quark
             production and decay, are B(t→uγ)<0.85(0.88−0.25+0.37)×10−5
             and B(t→cγ)<4.2(3.40−0.95+1.35)×10−5 for a
             left-handed tqγ coupling, and B(t→uγ)<1.2(1.20−0.33+0.50)×10−5
             and B(t→cγ)<4.5(3.70−1.03+1.47)×10−5 for a
             right-handed coupling.},
   Doi = {10.1016/j.physletb.2022.137379},
   Key = {fds372127}
}

@article{fds363185,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
             JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
             V and Arcangeletti, C},
   Title = {Search for flavour-changing neutral-current interactions of
             a top quark and a gluon in pp collisions at √s=13 TeV with
             the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {82},
   Number = {4},
   Year = {2022},
   Month = {April},
   url = {http://dx.doi.org/10.1140/epjc/s10052-022-10182-7},
   Abstract = {A search is presented for the production of a single top
             quark via left-handed flavour-changing neutral-current
             (FCNC) interactions of a top quark, a gluon and an up or
             charm quark. Two production processes are considered: u+
             g→ t and c+ g→ t. The analysis is based on
             proton–proton collision data taken at a centre-of-mass
             energy of 13 TeV with the ATLAS detector at the LHC. The
             data set corresponds to an integrated luminosity of 139 fb-
             1. Events with exactly one electron or muon, exactly one
             b-tagged jet and missing transverse momentum are selected,
             resembling the decay products of a singly produced top
             quark. Neural networks based on kinematic variables
             differentiate between events from the two signal processes
             and events from background processes. The measured data are
             consistent with the background-only hypothesis, and limits
             are set on the production cross-sections of the signal
             processes: σ(u+g→t)×B(t→Wb)×B(W→ℓν)<3.0pb and
             σ(c+g→t)×B(t→Wb)×B(W→ℓν)<4.7pb at the 95%
             confidence level, with B(W→ ℓν) = 0.325 being the sum
             of branching ratios of all three leptonic decay modes of the
             W boson. Based on the framework of an effective field
             theory, the cross-section limits are translated into limits
             on the strengths of the tug and tcg couplings occurring in
             the theory: |CuGut|/Λ2<0.057TeV- 2 and |CuGct|/Λ2<0.14TeV-
             2. These bounds correspond to limits on the branching ratios
             of FCNC-induced top-quark decays: B(t→ u+ g) < 0.61 × 10
             - 4 and B(t→ c+ g) < 3.7 × 10 - 4.},
   Doi = {10.1140/epjc/s10052-022-10182-7},
   Key = {fds363185}
}

@article{fds356623,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Search for four-top-quark production in the single-lepton
             and opposite-sign dilepton final states in pp collisions at
             s =13 TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {99},
   Number = {5},
   Year = {2019},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.99.052009},
   Abstract = {A search for four-top-quark production, tttt, is presented.
             It is based on proton-proton collision data with a
             center-of-mass energy s=13 TeV collected by the ATLAS
             detector at the Large Hadron Collider during the years 2015
             and 2016, corresponding to an integrated luminosity of 36.1
             fb-1. Data are analyzed in both the single-lepton and
             opposite-sign dilepton channels, characterized by the
             presence of one or two isolated electrons or muons with
             high-transverse momentum and multiple jets. A data-driven
             method is used to estimate the dominant background from
             top-quark pair production in association with jets. No
             significant excess above the Standard Model expectation is
             observed. The result is combined with the previous same-sign
             dilepton and multilepton searches carried out by the ATLAS
             Collaboration and an observed (expected) upper limit of 5.3
             (2.1) times the four-top-quark Standard Model cross section
             is obtained at 95% confidence level. Additionally, an upper
             limit on the anomalous four-top-quark production cross
             section is set in the context of an effective field theory
             model.},
   Doi = {10.1103/PhysRevD.99.052009},
   Key = {fds356623}
}

@article{fds307951,
   Author = {Aaltonen, T and others},
   Title = {Search for Gluino-Mediated Bottom Squark Production in
             p[overline p] Collisions at sqrt(s) = 1.96
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {22},
   Pages = {221801},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.221801},
   Abstract = {We report on a search for the supersymmetric partner of the
             bottom quark produced from gluino decays in data from 2.5
             fb;{-1} of integrated luminosity collected by the Collider
             Detector at Fermilab at sqrt[s]=1.96 TeV. Candidate events
             are selected requiring two or more jets and large missing
             transverse energy. At least two of the jets are required to
             be tagged as originating from a b quark to enhance the
             sensitivity. The results are in good agreement with the
             prediction of the standard model processes, giving no
             evidence for gluino decay to bottom squarks. This result
             constrains the gluino-pair-production cross section to be
             less than 40 fb at 95% credibility level for a gluino mass
             of 350 GeV/c;{2}.},
   Doi = {10.1103/physrevlett.102.221801},
   Key = {fds307951}
}

@article{fds321084,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako,
             K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
             EB and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner,
             M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji,
             W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer,
             F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin,
             S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
             P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet,
             D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret,
             MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini,
             I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli,
             R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro,
             NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas,
             CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Search for gluinos in events with an isolated lepton, jets
             and missing transverse momentum at [Formula: see text] = 13
             Te V with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {10},
   Pages = {565},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4397-x},
   Abstract = {The results of a search for gluinos in final states with an
             isolated electron or muon, multiple jets and large missing
             transverse momentum using proton-proton collision data at a
             centre-of-mass energy of [Formula: see text] are presented.
             The dataset used was recorded in 2015 by the ATLAS
             experiment at the Large Hadron Collider and corresponds to
             an integrated luminosity of 3.2 fb[Formula: see text]. Six
             signal selections are defined that best exploit the signal
             characteristics. The data agree with the Standard Model
             background expectation in all six signal selections, and the
             largest deviation is a 2.1 standard deviation excess. The
             results are interpreted in a simplified model where
             pair-produced gluinos decay via the lightest chargino to the
             lightest neutralino. In this model, gluinos are excluded up
             to masses of approximately 1.6 Te V depending on the mass
             spectrum of the simplified model, thus surpassing the limits
             of previous searches.},
   Doi = {10.1140/epjc/s10052-016-4397-x},
   Key = {fds321084}
}

@article{fds307699,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni,
             G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth,
             CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B},
   Title = {Search for gluinos in events with two same-sign leptons,
             jets, and missing transverse momentum with the ATLAS
             detector in pp collisions at sqrt[s]=7  TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {24},
   Pages = {241802},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.108.241802},
   Abstract = {A search is presented for gluinos decaying via the
             supersymmetric partner of the top quark using events with
             two same-sign leptons, jets, and missing transverse
             momentum. The analysis is performed with 2.05  fb(-1) of
             integrated luminosity from pp collisions at
             sqrt[s]=7  TeV collected by the ATLAS detector at the
             LHC. No excess beyond the standard model expectation is
             observed, and exclusion limits are derived for simplified
             models where the gluino decays via the supersymmetric
             partner of the top quark and in the minimal supergravity and
             constrained minimal supersymmetric standard model framework.
             In those scenarios, gluino masses below 550 GeV are excluded
             at 95% C.L. within the parameter space considered,
             significantly extending the coverage with respect to
             existing limits. Depending on the model parameters, gluino
             masses up to 750 GeV can also be excluded at 95%
             C.L.},
   Doi = {10.1103/physrevlett.108.241802},
   Key = {fds307699}
}

@article{fds307965,
   Author = {Aaltonen, T and others},
   Title = {Search for hadronic decays of W and Z bosons in photon
             events in pp̅ collisions at sqrt[s] =1.96
             TeV},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {5},
   Pages = {052011},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.052011},
   Abstract = {We report on a search for the process pp̅ →γ+W/Z with
             W/Z→qq̅ in events containing two jets and a photon at the
             center-of-mass energy sqrt[s]=1.96  TeV, using
             184  pb-1 of data collected by the CDF II detector. A
             neural network event selection has been developed to
             optimize the rejection of the large QCD production
             background; it is shown that this method gives a significant
             improvement in both signal-to-noise ratio and signal
             sensitivity, as compared with an event selection based on
             conventional cuts. An upper limit is presented for the
             γ+W/Z production cross section with the W and Z decaying
             hadronically.},
   Doi = {10.1103/PhysRevD.80.052011},
   Key = {fds307965}
}

@article{fds347475,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
             H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
             O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Li, C-Q and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and CalventeLopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho
             Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo,
             F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati,
             L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
             YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
             YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Search for heavy ZZ resonances in the ℓ + ℓ - ℓ
             + ℓ - and ℓ + ℓ - ν ν ¯ final states using
             proton-proton collisions at s = 13   TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {4},
   Pages = {293},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-5686-3},
   Abstract = {A search for heavy resonances decaying into a pair of Z
             bosons leading to ℓ + ℓ - ℓ + ℓ - and ℓ + ℓ - ν
             ν ¯ final states, where ℓ stands for either an electron
             or a muon, is presented. The search uses proton-proton
             collision data at a centre-of-mass energy of 13  TeV
             corresponding to an integrated luminosity of 36.1  fb - 1
             collected with the ATLAS detector during 2015 and 2016 at
             the Large Hadron Collider. Different mass ranges for the
             hypothetical resonances are considered, depending on the
             final state and model. The different ranges span between 200
             and 2000  GeV . The results are interpreted as upper limits
             on the production cross section of a spin-0 or spin-2
             resonance. The upper limits for the spin-0 resonance are
             translated to exclusion contours in the context of Type-I
             and Type-II two-Higgs-doublet models, while those for the
             spin-2 resonance are used to constrain the Randall-Sundrum
             model with an extra dimension giving rise to spin-2 graviton
             excitations.},
   Doi = {10.1140/epjc/s10052-018-5686-3},
   Key = {fds347475}
}

@article{fds307850,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for Heavy Bottomlike Quarks Decaying to an Electron
             or Muon and Jets in $p\overline{p}$ Collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {14},
   Pages = {141803},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.141803},
   Abstract = {We report the most sensitive direct search for pair
             production of fourth-generation bottomlike chiral quarks
             (b') each decaying promptly to tW. We search for an excess
             of events with an electron or muon, at least five jets (one
             identified as due to a b or c quark), and an imbalance of
             transverse momentum by using data from pp collisions
             collected by the CDF II detector at Fermilab with an
             integrated luminosity of 4.8  fb(-1). We observe events
             consistent with background expectation, calculate upper
             limits on the b' pair-production cross section (σ(bb'))
             ≲30  fb for m(b') > 375  GeV/c2), and exclude
             m(b') < 372  GeV/c2 at 95% confidence level assuming a
             100% branching ratio of b' to tW.},
   Doi = {10.1103/PhysRevLett.106.141803},
   Key = {fds307850}
}

@article{fds348657,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {Search for heavy charged long-lived particles in
             proton–proton collisions at √s=13TeV using an ionisation
             measurement with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {788},
   Pages = {96-116},
   Year = {2019},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.10.055},
   Abstract = {This Letter presents a search for heavy charged long-lived
             particles produced in proton–proton collisions at s=13TeV
             at the LHC using a data sample corresponding to an
             integrated luminosity of 36.1fb−1 collected by the ATLAS
             experiment in 2015 and 2016. These particles are expected to
             travel with a velocity significantly below the speed of
             light, and therefore have a specific ionisation higher than
             any high-momentum Standard Model particle of unit charge.
             The pixel subsystem of the ATLAS detector is used in this
             search to measure the ionisation energy loss of all
             reconstructed charged particles which traverse the pixel
             detector. Results are interpreted assuming the pair
             production of R-hadrons as composite colourless states of a
             long-lived gluino and Standard Model partons. No significant
             deviation from Standard Model background expectations is
             observed, and lifetime-dependent upper limits on R-hadron
             production cross-sections and gluino masses are set,
             assuming the gluino always decays to two quarks and a 100
             GeV stable neutralino. R-hadrons with lifetimes above 1.0 ns
             are excluded at the 95% confidence level, with lower limits
             on the gluino mass ranging between 1290 GeV and 2060 GeV. In
             the case of stable R-hadrons, the lower limit on the gluino
             mass at the 95% confidence level is 1890
             GeV.},
   Doi = {10.1016/j.physletb.2018.10.055},
   Key = {fds348657}
}

@article{fds356596,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA},
   Title = {Search for heavy charged long-lived particles in the ATLAS
             detector in 36.1 fb-1 of proton-proton collision data at s
             =13 TeV},
   Journal = {Physical Review D},
   Volume = {99},
   Number = {9},
   Year = {2019},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.99.092007},
   Abstract = {A search for heavy charged long-lived particles is performed
             using a data sample of 36.1 fb-1 of proton-proton collisions
             at s=13 TeV collected by the ATLAS experiment at the Large
             Hadron Collider. The search is based on observables related
             to ionization energy loss and time of flight, which are
             sensitive to the velocity of heavy charged particles
             traveling significantly slower than the speed of light.
             Multiple search strategies for a wide range of lifetimes,
             corresponding to path lengths of a few meters, are defined
             as model independently as possible, by referencing several
             representative physics cases that yield long-lived particles
             within supersymmetric models, such as gluinos/squarks
             (R-hadrons), charginos and staus. No significant deviations
             from the expected Standard Model background are observed.
             Upper limits at 95% confidence level are provided on the
             production cross sections of long-lived R-hadrons as well as
             directly pair-produced staus and charginos. These results
             translate into lower limits on the masses of long-lived
             gluino, sbottom and stop R-hadrons, as well as staus and
             charginos of 2000, 1250, 1340, 430, and 1090 GeV,
             respectively.},
   Doi = {10.1103/PhysRevD.99.092007},
   Key = {fds356596}
}

@article{fds354541,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
             MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
             CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti,
             C},
   Title = {Search for heavy diboson resonances in semileptonic final
             states in pp collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {12},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2020},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-08554-y},
   Abstract = {This paper reports on a search for heavy resonances decaying
             into WW, ZZ or WZ using proton–proton collision data at a
             centre-of-mass energy of s=13 TeV. The data, corresponding
             to an integrated luminosity of 139 fb 1, were recorded with
             the ATLAS detector from 2015 to 2018 at the Large Hadron
             Collider. The search is performed for final states in which
             one W or Z boson decays leptonically, and the other W boson
             or Z boson decays hadronically. The data are found to be
             described well by expected backgrounds. Upper bounds on the
             production cross sections of heavy scalar, vector or tensor
             resonances are derived in the mass range 300–5000 GeV
             within the context of Standard Model extensions with warped
             extra dimensions or including a heavy vector triplet.
             Production through gluon–gluon fusion, Drell–Yan or
             vector-boson fusion are considered, depending on the assumed
             model.},
   Doi = {10.1140/epjc/s10052-020-08554-y},
   Key = {fds354541}
}

@article{fds347487,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov,
             VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel,
             M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
             A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz,
             T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black,
             KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
             YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
             YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C},
   Title = {Search for Heavy Higgs Bosons A/H Decaying to a Top Quark
             Pair in pp Collisions at sqrt[s]=8  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {119},
   Number = {19},
   Pages = {191803},
   Year = {2017},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.119.191803},
   Abstract = {A search for heavy pseudoscalar (A) and scalar (H) Higgs
             bosons decaying into a top quark pair (tt[over ¯]) has been
             performed with 20.3  fb^{-1} of proton-proton collision
             data collected by the ATLAS experiment at the Large Hadron
             Collider at a center-of-mass energy sqrt[s]=8  TeV.
             Interference effects between the signal process and standard
             model tt[over ¯] production, which are expected to distort
             the signal shape from a single peak to a peak-dip structure,
             are taken into account. No significant deviation from the
             standard model prediction is observed in the tt[over ¯]
             invariant mass spectrum in final states with an electron or
             muon, large missing transverse momentum, and at least four
             jets. The results are interpreted within the context of a
             type-II two-Higgs-doublet model. Exclusion limits on the
             signal strength are derived as a function of the mass
             m_{A/H} and the ratio of the vacuum expectation values of
             the two Higgs fields, tanβ, for m_{A/H}>500  GeV.},
   Doi = {10.1103/physrevlett.119.191803},
   Key = {fds347487}
}

@article{fds351557,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei,
             V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Artz,
             S and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou,
             EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Avolio, G and Ayoub, MK and Azuelos, G and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani,
             H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker,
             OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour,
             G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton,
             AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso,
             MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
             P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya, DS and Bhattarai,
             P and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
             V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla,
             JS and Boonekamp, M and Booth, CD and Borecka-Bielska, HM and Borgna,
             LS and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
             DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
             G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Bruncko,
             D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez,
             CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba,
             LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero,
             J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney,
             RMD and Caron, S and Carquin, E and Carrá, S and Carter, JWS and Carter,
             TM and Casado, MP and Casha, AF and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavallaro, E and Cavasinni, V and Celebi,
             E and Celli, F and Cerda Alberich and L and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen,
             SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont,
             AR and Chouridou, S and Chow, YS and Christopher, LD and Chu, MC and Chu,
             X and Chudoba, J and Chwastowski, JJ and Chytka, L and Cieri,
             D},
   Title = {Search for Heavy Higgs Bosons Decaying into Two Tau Leptons
             with the ATLAS Detector Using pp Collisions at
             sqrt[s]=13  TeV.},
   Journal = {Physical review letters},
   Volume = {125},
   Number = {5},
   Pages = {051801},
   Year = {2020},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.125.051801},
   Abstract = {A search for heavy neutral Higgs bosons is performed using
             the LHC Run 2 data, corresponding to an integrated
             luminosity of 139  fb^{-1} of proton-proton collisions
             at sqrt[s]=13  TeV recorded with the ATLAS detector. The
             search for heavy resonances is performed over the mass range
             0.2-2.5 TeV for the τ^{+}τ^{-} decay with at least one
             τ-lepton decaying into final states with hadrons. The data
             are in good agreement with the background prediction of the
             standard model. In the M_{h}^{125} scenario of the minimal
             supersymmetric standard model, values of tanβ>8 and
             tanβ>21 are excluded at the 95% confidence level for
             neutral Higgs boson masses of 1.0 and 1.5 TeV,
             respectively, where tanβ is the ratio of the vacuum
             expectation values of the two Higgs doublets.},
   Doi = {10.1103/physrevlett.125.051801},
   Key = {fds351557}
}

@article{fds313595,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
             G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for heavy lepton resonances decaying to a Z boson and
             a lepton in pp collisions at s√=8},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {9},
   Pages = {1-38},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2015)108},
   Abstract = {A search for heavy leptons decaying to a Z boson and an
             electron or a muon is presented. The search is based on pp
             collision data taken at (Formula presented.) = 8 TeV by the
             ATLAS experiment at the CERN Large Hadron Collider,
             corresponding to an integrated luminosity of 20.3 fb−1.
             Three high-transverse-momentum electrons or muons are
             selected, with two of them required to be consistent with
             originating from a Z boson decay. No significant excess
             above Standard Model background predictions is observed, and
             95% confidence level limits on the production cross section
             of high-mass trilepton resonances are derived. The results
             are interpreted in the context of vector-like lepton and
             type-III seesaw models. For the vector-like lepton model,
             most heavy lepton mass values in the range 114–176 GeV are
             excluded. For the type-III seesaw model, most mass values in
             the range 100–468 GeV are excluded.},
   Doi = {10.1007/JHEP09(2015)108},
   Key = {fds313595}
}

@article{fds307865,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R and Ask, S},
   Title = {Search for heavy long-lived charged particles with the ATLAS
             detector in pp collisions at √s=7 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {703},
   Number = {4},
   Pages = {428-446},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.08.042},
   Abstract = {A search for long-lived charged particles reaching the muon
             spectrometer is performed using a data sample of 37 pb-1
             from pp collisions at √s=7 TeV collected by the ATLAS
             detector at the LHC in 2010. No excess is observed above the
             estimated background. Stable τ̃ sleptons are excluded at
             95% CL up to a mass of 136 GeV, in GMSB models with N5=3,
             mmessenger=250 TeV, sign(μ)=1 and tanβ=5. Electroweak
             production of sleptons is excluded up to a mass of 110 GeV.
             Gluino R-hadrons in a generic interaction model are excluded
             up to masses of 530 GeV to 544 GeV depending on the fraction
             of R-hadrons produced as g̃-balls. © 2011
             CERN.},
   Doi = {10.1016/j.physletb.2011.08.042},
   Key = {fds307865}
}

@article{fds321088,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adersberger, M and Adomeit, S and Adye,
             T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Search for heavy long-lived charged R-hadrons with the ATLAS
             detector in 3.2 fb−1 of proton–proton
             collision data at √s=13 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {760},
   Pages = {647-665},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.07.042},
   Abstract = {A search for heavy long-lived charged R-hadrons is reported
             using a data sample corresponding to 3.2 fb−1 of
             proton–proton collisions at s=13 TeV collected by the
             ATLAS experiment at the Large Hadron Collider at CERN. The
             search is based on observables related to large ionisation
             losses and slow propagation velocities, which are signatures
             of heavy charged particles travelling significantly slower
             than the speed of light. No significant deviations from the
             expected background are observed. Upper limits at 95%
             confidence level are provided on the production cross
             section of long-lived R-hadrons in the mass range from 600
             GeV to 2000 GeV and gluino, bottom and top squark masses are
             excluded up to 1580 GeV, 805 GeV and 890 GeV,
             respectively.},
   Doi = {10.1016/j.physletb.2016.07.042},
   Key = {fds321088}
}

@article{fds310334,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
             P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
             C},
   Title = {Search for heavy long-lived multi-charged particles in
             pp collisions at [Formula: see text] TeV using the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {8},
   Pages = {362},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3534-2},
   Abstract = {A search for heavy long-lived multi-charged particles is
             performed using the ATLAS detector at the LHC. Data
             collected in 2012 at [Formula: see text] TeV from <i>pp</i>
             collisions corresponding to an integrated luminosity of
             20.3 fb[Formula: see text]are examined. Particles producing
             anomalously high ionisation, consistent with long-lived
             massive particles with electric charges from [Formula: see
             text] to [Formula: see text] are searched for. No signal
             candidate events are observed, and 95 % confidence level
             cross-section upper limits are interpreted as lower mass
             limits for a Drell-Yan production model. The mass limits
             range between 660 and 785 GeV.},
   Doi = {10.1140/epjc/s10052-015-3534-2},
   Key = {fds310334}
}

@article{fds375877,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam
             Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos,
             KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E},
   Title = {Search for heavy long-lived multi-charged particles in the
             full LHC Run 2 pp collision data at s=13 TeV using the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {847},
   Year = {2023},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.138316},
   Abstract = {A search for heavy long-lived multi-charged particles is
             performed using the ATLAS detector at the LHC. Data
             collected in 2015–2018 at s=13 TeV from pp collisions
             corresponding to an integrated luminosity of 139 fb−1 are
             examined. Particles producing anomalously high ionization,
             consistent with long-lived spin-½ massive particles with
             electric charges from |q|=2e to |q|=7e are searched for. No
             statistically significant evidence of such particles is
             observed, and 95% confidence level cross-section upper
             limits are calculated and interpreted as the lower mass
             limits for a Drell–Yan plus photon-fusion production mode.
             The least stringent limit, 1060 GeV, is obtained for |q|=2e
             particles, and the most stringent one, 1600 GeV, is for
             |q|=6e particles.},
   Doi = {10.1016/j.physletb.2023.138316},
   Key = {fds375877}
}

@article{fds356622,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA},
   Title = {Search for heavy long-lived multicharged particles in
             proton-proton collisions at s =13 TeV using the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {99},
   Number = {5},
   Year = {2019},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.99.052003},
   Abstract = {A search for heavy long-lived multicharged particles is
             performed using the ATLAS detector at the LHC. Data with an
             integrated luminosity of 36.1 fb-1 collected in 2015 and
             2016 from proton-proton collisions at s=13 TeV are examined.
             Particles producing anomalously high ionization, consistent
             with long-lived massive particles with electric charges from
             |q|=2e to |q|=7e, are searched for. No events are observed,
             and 95% confidence level cross-section upper limits are
             interpreted as lower mass limits for a Drell-Yan production
             model. Multicharged particles with masses between 50 and
             980-1220 GeV (depending on their electric charge) are
             excluded.},
   Doi = {10.1103/PhysRevD.99.052003},
   Key = {fds356622}
}

@article{fds316568,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold,
             H},
   Title = {Search for heavy Majorana neutrinos with the ATLAS detector
             in pp collisions at √s = 8 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {7},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2015)162},
   Abstract = {Abstract: A search for heavy Majorana neutrinos in events
             containing a pair of high-pT leptons of the same charge and
             high-pT jets is presented. The search uses 20.3 fb−1 of pp
             collision data collected with the ATLAS detector at the CERN
             Large Hadron Collider with a centre-of-mass energy of 221as
             = 8 TeV. The data are found to be consistent with the
             background-only hypothesis based on the Standard Model
             expectation. In the context of a Type-I seesaw mechanism,
             limits are set on the production cross-section times
             branching ratio for production of heavy Majorana neutrinos
             in the mass range between 100 and 500 GeV. The limits are
             subsequently interpreted as limits on the mixing between the
             heavy Majorana neutrinos and the Standard Model neutrinos.
             In the context of a left-right symmetric model, limits on
             the production cross-section times branching ratio are set
             with respect to the masses of heavy Majorana neutrinos and
             heavy gauge bosons WR and Z′.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP07(2015)162},
   Key = {fds316568}
}

@article{fds375849,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel,
             A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed,
             WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh,
             B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
             AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung,
             C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Arcangeletti,
             C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Tame,
             ZPA and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten,
             K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Gupta, DB and Balasubramanian, R and Baldin,
             EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas,
             WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits,
             M-S and Barklow, T and Baron, P and Moreno, DAB and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Navarro, LB and Barreiro, F and da
             Costa, JBG and Barron, U and Teixeira, MGB and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Hurrell, LTB and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
             K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
             L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Kuutmann, EB and Berger, N and Bergmann, B and Beringer, J and Bernardi,
             G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta,
             P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
             V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Sola, JDB and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
             R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and de Renstrom, PAB and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
             CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Vazquez, CJB and Buzykaev, AR and Cabras, G and Urbán, SC and Caforio,
             D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba,
             LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Toro, RC and Camarda, S and Munoz, DC and Camarri, P and Camerlingo, MT and Cameron,
             D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Bret, MC and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson,
             BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Argos, FC and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia,
             EG and Castillo, FL and Garcia, LC and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
             J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Moursli, RCE and Cheu, E and Cheung, K and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi,
             K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron,
             ZH},
   Title = {Search for heavy Majorana or Dirac neutrinos and
             right-handed W gauge bosons in final states with charged
             leptons and jets in pp collisions at $$\sqrt{s}=13$$ TeV
             with the ATLAS detector},
   Journal = {The European Physical Journal C},
   Volume = {83},
   Number = {12},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2023},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-12021-9},
   Abstract = {<jats:title>Abstract</jats:title><jats:p>A search for heavy
             right-handed Majorana or Dirac neutrinos
             <jats:inline-formula><jats:alternatives><jats:tex-math>$$N_{\textrm{R}}$$</jats:tex-math>??
             <mml:msub> <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext>
             </mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
             and heavy right-handed gauge bosons <jats:inline-formula><jats:alternatives><jats:tex-math>$$W_{\textrm{R}}$$</jats:tex-math>??
             <mml:msub> <mml:mi>W</mml:mi> <mml:mtext>R</mml:mtext>
             </mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
             is performed in events with energetic electrons or muons,
             with the same or opposite electric charge, and energetic
             jets. The search is carried out separately for topologies of
             clearly separated final-state products (“resolved”
             channel) and topologies with boosted final states with
             hadronic and/or leptonic products partially overlapping and
             reconstructed as a large-radius jet (“boosted” channel).
             The events are selected from <jats:italic>pp</jats:italic>
             collision data at the LHC with an integrated luminosity of
             139 fb<jats:inline-formula><jats:alternatives><jats:tex-math>$$^{-1}$$</jats:tex-math>??
             <mml:msup> <mml:mrow /> <mml:mrow> <mml:mo>-</mml:mo>
             <mml:mn>1</mml:mn> </mml:mrow> </mml:msup>
             </mml:math></jats:alternatives></jats:inline-formula>
             collected by the ATLAS detector at <jats:inline-formula><jats:alternatives><jats:tex-math>$$\sqrt{s}
             = 13$$</jats:tex-math>?? <mml:mrow> <mml:msqrt>
             <mml:mi>s</mml:mi> </mml:msqrt> <mml:mo>=</mml:mo>
             <mml:mn>13</mml:mn> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> TeV.
             No significant deviations from the Standard Model
             predictions are observed. The results are interpreted within
             the theoretical framework of a left-right symmetric model,
             and lower limits are set on masses in the heavy right-handed
             <jats:inline-formula><jats:alternatives><jats:tex-math>$$W_{\textrm{R}}$$</jats:tex-math>??
             <mml:msub> <mml:mi>W</mml:mi> <mml:mtext>R</mml:mtext>
             </mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
             boson and <jats:inline-formula><jats:alternatives><jats:tex-math>$$N_{\textrm{R}}$$</jats:tex-math>??
             <mml:msub> <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext>
             </mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
             plane. The excluded region extends to about
             <jats:inline-formula><jats:alternatives><jats:tex-math>$$m(W_{\textrm{R}})
             = 6.4$$</jats:tex-math>?? <mml:mrow> <mml:mi>m</mml:mi>
             <mml:mo>(</mml:mo> <mml:msub> <mml:mi>W</mml:mi>
             <mml:mtext>R</mml:mtext> </mml:msub> <mml:mo>)</mml:mo>
             <mml:mo>=</mml:mo> <mml:mn>6.4</mml:mn> </mml:mrow>
             </mml:math></jats:alternatives></jats:inline-formula> TeV
             for both Majorana and Dirac <jats:inline-formula><jats:alternatives><jats:tex-math>$$N_{\textrm{R}}$$</jats:tex-math>??
             <mml:msub> <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext>
             </mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
             neutrinos at <jats:inline-formula><jats:alternatives><jats:tex-math>$$m(N_{\textrm{R}})&lt;1$$</jats:tex-math>??
             <mml:mrow> <mml:mi>m</mml:mi> <mml:mo>(</mml:mo> <mml:msub>
             <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext> </mml:msub>
             <mml:mo>)</mml:mo> <mml:mo>&lt;</mml:mo> <mml:mn>1</mml:mn>
             </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> TeV.
             <jats:inline-formula><jats:alternatives><jats:tex-math>$$N_{\textrm{R}}$$</jats:tex-math>??
             <mml:msub> <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext>
             </mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
             with masses of less than 3.5 (3.6) TeV are excluded in the
             electron (muon) channel at <jats:inline-formula><jats:alternatives><jats:tex-math>$$m(W_{\textrm{R}})=4.8$$</jats:tex-math>??
             <mml:mrow> <mml:mi>m</mml:mi> <mml:mo>(</mml:mo> <mml:msub>
             <mml:mi>W</mml:mi> <mml:mtext>R</mml:mtext> </mml:msub>
             <mml:mo>)</mml:mo> <mml:mo>=</mml:mo> <mml:mn>4.8</mml:mn>
             </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> TeV
             for the Majorana neutrinos, and limits of
             <jats:inline-formula><jats:alternatives><jats:tex-math>$$m(N_{\textrm{R}})$$</jats:tex-math>??
             <mml:mrow> <mml:mi>m</mml:mi> <mml:mo>(</mml:mo> <mml:msub>
             <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext> </mml:msub>
             <mml:mo>)</mml:mo> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula>
             up to 3.6 TeV for <jats:inline-formula><jats:alternatives><jats:tex-math>$$m(W_{\textrm{R}})
             = 5.2$$</jats:tex-math>?? <mml:mrow> <mml:mi>m</mml:mi>
             <mml:mo>(</mml:mo> <mml:msub> <mml:mi>W</mml:mi>
             <mml:mtext>R</mml:mtext> </mml:msub> <mml:mo>)</mml:mo>
             <mml:mo>=</mml:mo> <mml:mn>5.2</mml:mn> </mml:mrow>
             </mml:math></jats:alternatives></jats:inline-formula>
             (5.0) TeV in the electron (muon) channel are set for the
             Dirac neutrinos. These constitute the most stringent
             exclusion limits to date for the model considered.</jats:p>},
   Doi = {10.1140/epjc/s10052-023-12021-9},
   Key = {fds375849}
}

@article{fds347450,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Search for heavy Majorana or Dirac neutrinos and
             right-handed W gauge bosons in final states with two charged
             leptons and two jets at √s=13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {1},
   Year = {2019},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2019)016},
   Abstract = {A search for heavy right-handed Majorana or Dirac neutrinos
             NR and heavy right-handed gauge bosons WR is performed in
             events with a pair of energetic electrons or muons, with the
             same or opposite electric charge, and two energetic jets.
             The events are selected from pp collision data with an
             integrated luminosity of 36.1 fb−1 collected by the ATLAS
             detector at s=13 TeV. No significant deviations from the
             Standard Model are observed. The results are interpreted
             within the theoretical framework of a left-right symmetric
             model and lower limits are set on masses in the heavy
             right-handed W boson and neutrino mass plane. The excluded
             region extends to mRR=4.7 TeV for both Majorana and Dirac NR
             neutrinos.},
   Doi = {10.1007/JHEP01(2019)016},
   Key = {fds347450}
}

@article{fds307804,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R},
   Title = {Search for heavy metastable particles decaying to jet pairs
             in pp̄ collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012007},
   Abstract = {A search is performed for heavy metastable particles that
             decay into jet pairs with a macroscopic lifetime (cτ∼1cm)
             in pp̄ collisions at √s=1.96TeV using data from the CDF
             II detector at Fermilab corresponding to an integrated
             luminosity of 3.2fb-1. To estimate the standard model
             background, a data-driven approach is used.
             Probability-density functions are constructed to model
             secondary vertices from known processes. No statistically
             significant excess is observed above the background. Limits
             on the production cross section in a hidden valley benchmark
             phenomenology are set for various Higgs boson masses as well
             as metastable particle masses and lifetimes. © 2012
             American Physical Society.},
   Doi = {10.1103/PhysRevD.85.012007},
   Key = {fds307804}
}

@article{fds353483,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
             V},
   Title = {Search for heavy neutral Higgs bosons produced in
             association with b-quarks and decaying into b-quarks at s
             =13 TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {102},
   Number = {3},
   Year = {2020},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.102.032004},
   Abstract = {A search for heavy neutral Higgs bosons produced in
             association with one or two b-quarks and decaying to b-quark
             pairs is presented using 27.8 fb-1 of s=13 TeV proton-proton
             collision data recorded by the ATLAS detector at the Large
             Hadron Collider during 2015 and 2016. No evidence of a
             signal is found. Upper limits on the heavy neutral Higgs
             boson production cross section times its branching ratio to
             bb¯ are set, ranging from 4.0 to 0.6 pb at 95% confidence
             level over a Higgs boson mass range of 450 to 1400 GeV.
             Results are interpreted within the two-Higgs-doublet model
             and the minimal supersymmetric Standard Model.},
   Doi = {10.1103/PhysRevD.102.032004},
   Key = {fds353483}
}

@article{fds356571,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
             V},
   Title = {Search for heavy neutral leptons in decays of W bosons
             produced in 13 TeV pp collisions using prompt and displaced
             signatures with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {10},
   Year = {2019},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2019)265},
   Abstract = {The problems of neutrino masses, matter-antimatter
             asymmetry, and dark matter could be successfully addressed
             by postulating right-handed neutrinos with Majorana masses
             below the electroweak scale. In this work, leptonic decays
             of W bosons extracted from 32.9 fb−1 to 36.1 fb−1 of 13
             TeV proton–proton collisions at the LHC are used to search
             for heavy neutral leptons (HNLs) that are produced through
             mixing with muon or electron neutrinos. The search is
             conducted using the ATLAS detector in both prompt and
             displaced leptonic decay signatures. The prompt signature
             requires three leptons produced at the interaction point
             (either μμe or eeμ) with a veto on same-flavour
             opposite-charge topologies. The displaced signature
             comprises a prompt muon from the W boson decay and the
             requirement of a dilepton vertex (either μμ or μe)
             displaced in the transverse plane by 4–300 mm from the
             interaction point. The search sets constraints on the HNL
             mixing to muon and electron neutrinos for HNL masses in the
             range 4.5–50 GeV. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP10(2019)265},
   Key = {fds356571}
}

@article{fds372388,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
             JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
             M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Austrup, VA and Avner, G and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari,
             T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baroncelli, A and Barone, G and Barr, AJ and Barranco
             Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini,
             G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
             K and Becot, C and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos,
             P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun,
             D and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
             Kuutmann, E and Berger, N and Bergmann, B and Beringer, J and Berlendis,
             S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Bethke, S and Betti, A and Bevan, AJ and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes,
             CJ and Bird, GA and Birman, M and Bisanz, T and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler, S and Brickwedde,
             B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks,
             WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko,
             D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard,
             CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler,
             JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez,
             CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura,
             P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet,
             D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
             JCJ and Cardillo, F and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin,
             E and Carrá, S and Carratta, G and Carter, JWS and Carter, TM and Casadei,
             D and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
             DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
             YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
             BM and Clark, A and Clark, PJ and Clavijo Columbie and JM and Clawson, SE and Clement, C and Clissa, L and Coadou, Y and Cobal,
             M},
   Title = {Search for Heavy Neutral Leptons in Decays of W Bosons Using
             a Dilepton Displaced Vertex in sqrt[s]=13  TeV pp
             Collisions with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {131},
   Number = {6},
   Pages = {061803},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.131.061803},
   Abstract = {A search for a long-lived, heavy neutral lepton (N) in
             139  fb^{-1} of sqrt[s]=13  TeV pp collision data
             collected by the ATLAS detector at the Large Hadron Collider
             is reported. The N is produced via W→Nμ or W→Ne and
             decays into two charged leptons and a neutrino, forming a
             displaced vertex. The N mass is used to discriminate between
             signal and background. No signal is observed, and limits are
             set on the squared mixing parameters of the N with the
             left-handed neutrino states for the N mass range
             3  GeV<m_{N}<15  GeV. For the first time, limits are
             given for both single-flavor and multiflavor mixing
             scenarios motivated by neutrino flavor oscillation results
             for both the normal and inverted neutrino-mass
             hierarchies.},
   Doi = {10.1103/physrevlett.131.061803},
   Key = {fds372388}
}

@article{fds307723,
   Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C},
   Title = {Search for heavy neutrinos and right-handed W bosons
             in events with two leptons and jets in pp collisions
             at [Formula: see text] with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {72},
   Number = {7},
   Pages = {2056},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2056-4},
   Abstract = {This letter reports on a search for hypothetical heavy
             neutrinos, <i>N</i>, and right-handed gauge bosons,
             <i>W</i><sub>R</sub>, in events with high transverse
             momentum objects which include two reconstructed leptons and
             at least one hadronic jet. The results were obtained from
             data corresponding to an integrated luminosity of
             2.1 fb<sup>-1</sup> collected in proton-proton collisions
             at [Formula: see text] with the ATLAS detector at the CERN
             Large Hadron Collider. No excess above the Standard Model
             background expectation is observed. Excluded mass regions
             for Majorana and Dirac neutrinos are presented using two
             approaches for interactions that violate lepton and
             lepton-flavor numbers. One approach uses an effective
             operator framework, the other approach is guided by the
             Left-Right Symmetric Model. The results described in this
             letter represent the most stringent limits to date on the
             masses of heavy neutrinos and <i>W</i><sub>R</sub> bosons
             obtained in direct searches.},
   Doi = {10.1140/epjc/s10052-012-2056-4},
   Key = {fds307723}
}

@article{fds356598,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA},
   Title = {Search for heavy particles decaying into a top-quark pair in
             the fully hadronic final state in pp collisions at s =13 TeV
             with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {99},
   Number = {9},
   Year = {2019},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.99.092004},
   Abstract = {A search for new particles decaying into a pair of top
             quarks is performed using proton-proton collision data
             recorded with the ATLAS detector at the Large Hadron
             Collider at a center-of-mass energy of s=13 TeV
             corresponding to an integrated luminosity of 36.1 fb-1.
             Events consistent with top-quark pair production and the
             fully hadronic decay mode of the top quarks are selected by
             requiring multiple high transverse momentum jets including
             those containing b-hadrons. Two analysis techniques,
             exploiting dedicated top-quark pair reconstruction in
             different kinematic regimes, are used to optimize the search
             sensitivity to new hypothetical particles over a wide mass
             range. The invariant mass distribution of the two
             reconstructed top-quark candidates is examined for resonant
             production of new particles with various spins and decay
             widths. No significant deviation from the Standard Model
             prediction is observed and limits are set on the production
             cross-section times branching fraction for new hypothetical
             Z′ bosons, dark-matter mediators, Kaluza-Klein gravitons
             and Kaluza-Klein gluons. By comparing with the predicted
             production cross sections, the Z′ boson in the
             topcolor-assisted-technicolor model is excluded for masses
             up to 3.1-3.6 TeV, the dark-matter mediators in a simplified
             framework are excluded in the mass ranges from 0.8 to 0.9
             TeV and from 2.0 to 2.2 TeV, and the Kaluza-Klein gluon is
             excluded for masses up to 3.4 TeV, depending on the decay
             widths of the particles.},
   Doi = {10.1103/PhysRevD.99.092004},
   Key = {fds356598}
}

@article{fds310120,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev,
             VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett,
             JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MA and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del
             Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
             T and Feher, S and Fein, D and Ferbel, T and Filthaut, F and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin,
             R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grünendahl, S and Gupta,
             A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hildreth, MD and Hirosky,
             R and Hobbs, JD and Hoeneisen, B and Huang, Y and Illingworth, R and Ito,
             AS and Jaffré, M and Jain, S and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Kalinin, AM and Karmanov, D and Karmgard, D and Kehoe, R and Kharchilava, A and Kim, SK and Klima, B and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov,
             AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krivkova, P and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kuznetsov, VE and Landsberg, G and Leflat, A and Leggett, C and Lehner, F and Li, J and Li, QZ and Lima, JG and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AK and Madaras, RJ and Malyshev, VL and Manankov, V and Mao, HS and Marshall, T and Martin, MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy, R and McDonald, J and McMahon, T and Melanson, HL and Merkin, M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mokhov, N and Mondal,
             NK and Montgomery, HE and Moore, RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Nunnemann, T and O'Neil, D and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou, K and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Pétroff, P and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Qian, J and Raja, R and Rajagopalan,
             S and Ramberg, E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Sabirov, BM and Santoro, A and Sawyer,
             L and Schamberger, RD and Schellman, H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell,
             RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery,
             P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Strovink, M and Stutte, L and Sznajder,
             A and Taylor, W and Tentindo-Repond, S and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and van Gemmeren, P and Vaniev, V and Van
             Kooten, R and Varelas, N and Vertogradov, LS and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Womersley, J and Wood, DR and Yamada, R and Yamin, P and Yasuda, T and Yatsunenko, YA and Yip, K and Youssef, S and Yu, J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev, EG and Zylberstejn,
             A},
   Title = {Search for heavy particles decaying into electron-positron
             pairs in pp collisions.},
   Journal = {Physical review letters},
   Volume = {87},
   Number = {6},
   Pages = {061802},
   Year = {2001},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.87.061802},
   Abstract = {We present results of searches for technirho (rho(T)),
             techniomega (omega(T)), and Z' particles, using the decay
             channels rho(T),omega(T),Z'-->e(+)e(-). The search is based
             on 124.8 pb(-1) of data collected by the D0 detector at the
             Fermilab Tevatron during 1992-1996. In the absence of a
             signal, we set 95% C.L. upper limits on the cross sections
             for the processes pp-->rho(T),omega(T),Z'-->e(+)e(-) as a
             function of the mass of the decaying particle. For certain
             model parameters, we exclude the existence of degenerate
             rho(T) and omega(T) states with masses below about 200 GeV.
             We exclude a Z' with mass below 670 GeV, assuming that it
             has the same couplings to fermions as the Z
             boson.},
   Doi = {10.1103/physrevlett.87.061802},
   Key = {fds310120}
}

@article{fds336450,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik,
             Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Pereira, RA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
             M and Baker, OK and Bakker, PJ and Gupta, DB and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee,
             S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
             A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary,
             O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund,
             O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
             KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JSB and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt,
             A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
             DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
             D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, DC and Chan, SK and Chan,
             WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, J and Chen, S and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard,
             AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Clark, A},
   Title = {Search for heavy particles decaying into top-quark pairs
             using lepton-plus-jets events in proton-proton collisions at
             s = 13   TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {7},
   Pages = {565},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-5995-6},
   Abstract = {A search for new heavy particles that decay into top-quark
             pairs is performed using data collected from proton-proton
             collisions at a centre-of-mass energy of 13  TeV by the
             ATLAS detector at the Large Hadron Collider. The integrated
             luminosity of the data sample is 36.1 fb - 1 . Events
             consistent with top-quark pair production are selected by
             requiring a single isolated charged lepton, missing
             transverse momentum and jet activity compatible with a
             hadronic top-quark decay. Jets identified as likely to
             contain <i>b</i>-hadrons are required to reduce the
             background from other Standard Model processes. The
             invariant mass spectrum of the candidate top-quark pairs is
             examined for local excesses above the background
             expectation. No significant deviations from the Standard
             Model predictions are found. Exclusion limits are set on the
             production cross-section times branching ratio for
             hypothetical Z ' bosons, Kaluza-Kein gluons and Kaluza-Klein
             gravitons that decay into top-quark pairs.},
   Doi = {10.1140/epjc/s10052-018-5995-6},
   Key = {fds336450}
}

@booklet{Abbott98f,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
             EW and Astur, R and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
             K and De, K and Del-Signore, K and Demarteau, M and Denisov, D and Denisov,
             SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
             Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {Search for heavy pointlike dirac monopoles},
   Journal = {Physical Review Letters},
   Volume = {81},
   Number = {3},
   Pages = {524-529},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.81.524},
   Abstract = {We have searched for central production of a pair of photons
             with high transverse energies in pp̄ collisions at √s=1.8
             TeV using 70pb-1 of data collected with the D0 detector at
             the Fermilab Tevatron in 1994-1996. If they exist virtual
             heavy pointlike Dirac monopoles could rescatter pairs of
             nearly real photons into this final state via a box diagram.
             We observe no excess of events above background and set
             lower 95% C.L. limits of 610 870 or 1580 GeV/c2 on the mass
             of a spin 0 1/2 or 1 Dirac monopole. © 1998 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.81.524},
   Key = {Abbott98f}
}

@article{fds347463,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
             P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
             JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
             H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
             C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
             AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
             O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
             S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
             R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
             JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Colasurdo,
             L},
   Title = {Search for heavy resonances decaying into WW in the e
             ν μ ν final state in pp collisions at s = 13 TeV
             with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {1},
   Pages = {24},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5491-4},
   Abstract = {A search for neutral heavy resonances is performed in the W
             W → e ν μ ν decay channel using <i>pp</i> collision
             data corresponding to an integrated luminosity of 36.1 fb -
             1 , collected at a centre-of-mass energy of 13 TeV by the
             ATLAS detector at the Large Hadron Collider. No evidence of
             such heavy resonances is found. In the search for production
             via the quark-antiquark annihilation or gluon-gluon fusion
             process, upper limits on σ X × B ( X → W W ) as a
             function of the resonance mass are obtained in the mass
             range between 200 GeV and up to 5 TeV for various benchmark
             models: a Higgs-like scalar in different width scenarios, a
             two-Higgs-doublet model, a heavy vector triplet model, and a
             warped extra dimensions model. In the vector-boson fusion
             process, constraints are also obtained on these resonances,
             as well as on a Higgs boson in the Georgi-Machacek model and
             a heavy tensor particle coupling only to gauge
             bosons.},
   Doi = {10.1140/epjc/s10052-017-5491-4},
   Key = {fds347463}
}

@article{fds356047,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
             M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
   Title = {Search for heavy resonances decaying into a pair of Z bosons
             in the ℓ+-′
             +′ - and ℓ+-νν¯
             final states using 139 fb - 1 of proton–proton
             collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {4},
   Year = {2021},
   Month = {April},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09013-y},
   Abstract = {A search for heavy resonances decaying into a pair of Z
             bosons leading to ℓ+ℓ-ℓ′ +ℓ′ - and
             ℓ+ℓ-νν¯ final states, where ℓ stands for either an
             electron or a muon, is presented. The search uses
             proton–proton collision data at a centre-of-mass energy of
             13 TeV collected from 2015 to 2018 that corresponds to the
             integrated luminosity of 139 fb - 1 recorded by the ATLAS
             detector during Run 2 of the Large Hadron Collider.
             Different mass ranges spanning 200 GeV to 2000 GeV for the
             hypothetical resonances are considered, depending on the
             final state and model. In the absence of a significant
             observed excess, the results are interpreted as upper limits
             on the production cross section of a spin-0 or spin-2
             resonance. The upper limits for the spin-0 resonance are
             translated to exclusion contours in the context of Type-I
             and Type-II two-Higgs-doublet models, and the limits for the
             spin-2 resonance are used to constrain the Randall–Sundrum
             model with an extra dimension giving rise to spin-2 graviton
             excitations.},
   Doi = {10.1140/epjc/s10052-021-09013-y},
   Key = {fds356047}
}

@article{fds355022,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling,
             J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith,
             L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani,
             H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker,
             OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Balli, F and Balunas,
             WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett,
             RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr,
             AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bawa,
             HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold,
             A and Bertram, IA and Bessidskaia Bylund and O and Besson, N and Bethani,
             A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya,
             DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel,
             O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman, M and Bisanz, T and Biswal,
             JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Blazek,
             T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden
             Madden, WD and Brendlinger, K and Brener, R and Brenner, L and Brenner,
             R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr,
             JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti,
             P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati,
             L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carratta,
             G and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli, F and Cerny,
             K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
             DG and Charman, TP and Chatterjee, M and Chau, CC and Che, S and Chekanov,
             S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen,
             Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias,
             TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chow, YS and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ},
   Title = {Search for Heavy Resonances Decaying into a Photon and a
             Hadronically Decaying Higgs Boson in pp Collisions at
             sqrt[s]=13  TeV with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {125},
   Number = {25},
   Pages = {251802},
   Year = {2020},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.125.251802},
   Abstract = {This Letter presents a search for the production of new
             heavy resonances decaying into a Higgs boson and a photon
             using proton-proton collision data at sqrt[s]=13  TeV
             collected by the ATLAS detector at the LHC. The data
             correspond to an integrated luminosity of 139  fb^{-1}.
             The analysis is performed by reconstructing hadronically
             decaying Higgs boson (H→bb[over ¯]) candidates as single
             large-radius jets. A novel algorithm using information about
             the jet constituents in the center-of-mass frame of the jet
             is implemented to identify the two b quarks in the single
             jet. No significant excess of events is observed above the
             expected background. Upper limits are set on the production
             cross-section times branching fraction for narrow spin-1
             resonances decaying into a Higgs boson and a photon in the
             resonance mass range from 0.7 to 4 TeV, cross-section times
             branching fractions are excluded between 11.6 fb and
             0.11 fb at a 95% confidence level.},
   Doi = {10.1103/physrevlett.125.251802},
   Key = {fds355022}
}

@article{fds336455,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for heavy resonances decaying into a W or Z boson and
             a Higgs boson in final states with leptons and b-jets in 36
             fb−1 of √s=13 TeV pp collisions with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2018},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2018)174},
   Abstract = {A search is conducted for new resonances decaying into a W
             or Z boson and a 125 GeV Higgs boson in the νν¯ bb¯ ,
             ℓ±νbb¯ , and ℓ+ℓ−bb¯ final states, where ℓ± =
             e± or μ±, in pp collisions at s=13 TeV. The data used
             correspond to a total integrated luminosity of 36.1 fb−1
             collected with the ATLAS detector at the Large Hadron
             Collider during the 2015 and 2016 data-taking periods. The
             search is conducted by examining the reconstructed invariant
             or transverse mass distributions of W h and Zh candidates
             for evidence of a localised excess in the mass range of 220
             GeV up to 5 TeV. No significant excess is observed and the
             results are interpreted in terms of constraints on the
             production cross-section times branching fraction of heavy
             W′ and Z′ resonances in heavy-vector-triplet models and
             the CP-odd scalar boson A in two-Higgs-doublet models. Upper
             limits are placed at the 95% confidence level and range
             between 9.0 × 10−4 pb and 7.3 × 10−1 pb depending on
             the model and mass of the resonance.[Figure not available:
             see fulltext.].},
   Doi = {10.1007/JHEP03(2018)174},
   Key = {fds336455}
}

@article{fds356672,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for heavy resonances decaying to a photon and a
             hadronically decaying Z /W /H boson in pp collisions at s
             =13 TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {3},
   Year = {2018},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.032015},
   Abstract = {Many extensions of the Standard Model predict new resonances
             decaying to a Z, W, or Higgs boson and a photon. This paper
             presents a search for such resonances produced in pp
             collisions at s=13 TeV using a data set with an integrated
             luminosity of 36.1 fb-1 collected by the ATLAS detector at
             the LHC. The Z/W/H bosons are identified through their
             decays to hadrons. The data are found to be consistent with
             the Standard Model expectation in the entire investigated
             mass range. Upper limits are set on the production cross
             section times branching fraction for resonance decays to
             Z/W+γ in the mass range from 1.0 to 6.8 TeV and for the
             first time into H+γ in the mass range from 1.0 to 3.0
             TeV.},
   Doi = {10.1103/PhysRevD.98.032015},
   Key = {fds356672}
}

@article{fds356723,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
             LJ},
   Title = {Search for heavy resonances decaying to a W or Z boson and a
             Higgs boson in the qq¯(′)bb¯ final state in
             pp collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {774},
   Pages = {494-515},
   Year = {2017},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2017.09.066},
   Abstract = {A search for heavy resonances decaying to a W or Z boson and
             a Higgs boson in the qq¯(′)bb¯ final state is described.
             The search uses 36.1 fb−1 of proton–proton collision
             data at s=13 TeV collected by the ATLAS detector at the CERN
             Large Hadron Collider in 2015 and 2016. The data are in
             agreement with the Standard Model expectations, with the
             largest excess found at a resonance mass of 3.0 TeV with a
             local (global) significance of 3.3 (2.1) σ. The results are
             presented in terms of constraints on a simplified model with
             a heavy vector triplet. Upper limits are set on the
             production cross-section times branching ratio for
             resonances decaying to a W (Z) boson and a Higgs boson,
             itself decaying to bb¯, in the mass range between 1.1 and
             3.8 TeV at 95% confidence level; the limits range between 83
             and 1.6 fb (77 and 1.1 fb) at 95% confidence
             level.},
   Doi = {10.1016/j.physletb.2017.09.066},
   Key = {fds356723}
}

@article{fds356765,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for heavy resonances decaying to a Z boson and a
             photon in pp collisions at s=13 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {764},
   Pages = {11-30},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.11.005},
   Abstract = {This Letter presents a search for new resonances with mass
             larger than 250 GeV, decaying to a Z boson and a photon. The
             dataset consists of an integrated luminosity of 3.2 fb−1
             of pp collisions collected at s=13 TeV with the ATLAS
             detector at the Large Hadron Collider. The Z bosons are
             identified through their decays either to charged, light,
             lepton pairs (e+e−, μ+μ−) or to hadrons. The data are
             found to be consistent with the expected background in the
             whole mass range investigated and upper limits are set on
             the production cross section times decay branching ratio to
             Zγ of a narrow scalar boson with mass between 250 GeV and
             2.75 TeV.},
   Doi = {10.1016/j.physletb.2016.11.005},
   Key = {fds356765}
}

@article{fds307771,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
             A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
             JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and BenAmi, S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Böser, S and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik,
             J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada,
             LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido,
             MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino,
             G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya,
             GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Cataneo, F and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J},
   Title = {Search for heavy vector-like quarks coupling to light quarks
             in proton-proton collisions at √s=7 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {712},
   Number = {1-2},
   Pages = {22-39},
   Publisher = {Elsevier BV},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.03.082},
   Abstract = {This Letter presents a search for singly produced
             vector-like quarks, Q, coupling to light quarks, q. The
             search is sensitive to both charged current (CC) and neutral
             current (NC) processes, pp→Qq→Wqq' and pp→Qq→Zqq'
             with a leptonic decay of the vector gauge boson. In 1.04fb-1
             of data taken in 2011 by the ATLAS experiment at a
             center-of-mass energy √s=7 TeV, no evidence of such heavy
             vector-like quarks is observed above the expected Standard
             Model background. Limits on the heavy vector-like quark
             production cross section times branching ratio as a function
             of mass mQ are obtained. For a coupling κqQ=v/mQ, where v
             is the Higgs vacuum expectation value, 95% C.L. lower limits
             on the mass of a vector-like quark are set at 900 GeV and
             760 GeV from CC and NC processes, respectively. © 2012
             CERN.},
   Doi = {10.1016/j.physletb.2012.03.082},
   Key = {fds307771}
}

@article{fds308053,
   Author = {Abulencia, and A, and others},
   Title = {Search for heavy, long-lived particles that decay to photons
             at CDF II},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {12},
   Pages = {121801},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.99.121801},
   Abstract = {We present the first search for heavy, long-lived particles
             that decay to photons at a hadron collider. We use a sample
             of gamma+jet+missing transverse energy events in p[overline
             p] collisions at sqrt(s)=1.96 TeV taken with the CDF II
             detector. Candidate events are selected based on the arrival
             time of the photon at the detector. Using an integrated
             luminosity of 570 pb-1 of collision data, we observe 2
             events, consistent with the background estimate of
             1.3$\pm$0.7 events. While our search strategy does not rely
             on model-specific dynamics, we set cross section limits in a
             supersymmetric model with chi-tilde10-->gammaG-tilde and
             place the world-best 95\% C.L. lower limit on the
             chi-tilde10 mass of 101 GeV/c2 at tauchi-tilde[sub 1][sup
             0]=5 ns.},
   Doi = {10.1103/physrevlett.99.121801},
   Key = {fds308053}
}

@article{fds375048,
   Author = {A.V. Kotwal and the ATLAS Collaboration},
   Title = {Search for heavy, long-lived, charged particles with large
             ionisation energy loss in pp collisions at √s = 13 TeV
             using the ATLAS experiment and the full Run 2
             dataset},
   Volume = {2023},
   Number = {158},
   Publisher = {Journal of High Energy Physics},
   Year = {2023},
   Month = {June},
   url = {http://dx.doi.org/https://doi.org/10.1007/JHEP06(2023)158},
   Doi = {https://doi.org/10.1007/JHEP06(2023)158},
   Key = {fds375048}
}

@article{fds310298,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C},
   Title = {Search for Higgs and Z Boson Decays to J/ψγ and ϒ(nS)γ
             with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {12},
   Pages = {121801},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.114.121801},
   Abstract = {A search for the decays of the Higgs and Z bosons to J/ψγ
             and ϒ(nS)γ (n=1,2,3) is performed with pp collision data
             samples corresponding to integrated luminosities of up to
             20.3  fb^{-1} collected at sqrt[s]=8  TeV with the
             ATLAS detector at the CERN Large Hadron Collider. No
             significant excess of events is observed above expected
             backgrounds and 95% C.L. upper limits are placed on the
             branching fractions. In the J/ψγ final state the limits
             are 1.5×10^{-3} and 2.6×10^{-6} for the Higgs and Z boson
             decays, respectively, while in the ϒ(1S,2S,3S)γ final
             states the limits are (1.3,1.9,1.3)×10^{-3} and
             (3.4,6.5,5.4)×10^{-6}, respectively.},
   Doi = {10.1103/physrevlett.114.121801},
   Key = {fds310298}
}

@article{fds321089,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
             K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
             J and Billoud, TRV and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
             Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M},
   Title = {Search for Higgs and Z Boson Decays to ϕγ with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {117},
   Number = {11},
   Pages = {111802},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevlett.117.111802},
   Abstract = {A search for the decays of the Higgs and Z bosons to a ϕ
             meson and a photon is performed with a pp collision data
             sample corresponding to an integrated luminosity of
             2.7  fb^{-1} collected at sqrt[s]=13  TeV with the
             ATLAS detector at the LHC. No significant excess of events
             is observed above the background, and 95% confidence level
             upper limits on the branching fractions of the Higgs and Z
             boson decays to ϕγ of 1.4×10^{-3} and 8.3×10^{-6},
             respectively, are obtained.},
   Doi = {10.1103/physrevlett.117.111802},
   Key = {fds321089}
}

@article{fds356617,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Search for Higgs boson decays into a pair of light bosons in
             the bbμμ final state in pp collision at √s=13TeV with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {790},
   Pages = {1-21},
   Year = {2019},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.10.073},
   Abstract = {A search for decays of the Higgs boson into a pair of new
             spin-zero particles, H→aa, where the a-bosons decay into a
             b-quark pair and a muon pair, is presented. The search uses
             36.1 fb−1 of proton–proton collision data at s=13 TeV
             recorded by the ATLAS experiment at the LHC in 2015 and
             2016. No significant deviation from the Standard Model
             prediction is observed. Upper limits at 95% confidence level
             are placed on the branching ratio (σH/σSM)×B(H→aa→bbμμ),
             ranging from 1.2×10−4 to 8.4×10−4 in the a-boson mass
             range of 20–60 GeV. Model-independent limits are set on
             the visible production cross-section times the branching
             ratio to the bbμμ final state for new physics,
             σvis(X)×B(X→bbμμ), ranging from 0.1 fb to 0.73 fb for
             mμμ between 18 and 62 GeV.},
   Doi = {10.1016/j.physletb.2018.10.073},
   Key = {fds356617}
}

@article{fds354095,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling,
             J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asai, K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith,
             L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani,
             H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker,
             OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
             E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak,
             L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya, DS and Bhattarai,
             P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann,
             D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman, M and Bisanz, T and Biswal, JP and Biswas,
             D and Bitadze, A and Bittrich, C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bogavac, D and Bogdanchikov,
             AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock,
             I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman
             de Renstrom, PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr,
             JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti,
             P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati,
             L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carratta,
             G and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castillo,
             FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavallaro, E and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christopher,
             LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Chytka,
             L},
   Title = {Search for Higgs Boson Decays into a Z Boson and a Light
             Hadronically Decaying Resonance Using 13 TeV pp Collision
             Data from the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {125},
   Number = {22},
   Pages = {221802},
   Year = {2020},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.125.221802},
   Abstract = {A search for Higgs boson decays into a Z boson and a light
             resonance in two-lepton plus jet events is performed, using
             a pp collision dataset with an integrated luminosity of
             139  fb^{-1} collected at sqrt[s]=13  TeV by the
             ATLAS experiment at the CERN LHC. The resonance considered
             is a light boson with a mass below 4 GeV from a possible
             extended scalar sector or a charmonium state. Multivariate
             discriminants are used for the event selection and for
             evaluating the mass of the light resonance. No excess of
             events above the expected background is found. Observed
             (expected) 95% confidence-level upper limits are set on the
             Higgs boson production cross section times branching
             fraction to a Z boson and the signal resonance, with values
             in the range 17-340 pb (16_{-5}^{+6}-320_{-90}^{+130}  pb)
             for the different light spin-0 boson mass and branching
             fraction hypotheses, and with values of 110 and 100 pb
             (100_{-30}^{+40} and 100_{-30}^{+40}  pb) for the η_{c}
             and J/ψ hypotheses, respectively.},
   Doi = {10.1103/physrevlett.125.221802},
   Key = {fds354095}
}

@article{fds356674,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
             M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for Higgs boson decays into pairs of light
             (pseudo)scalar particles in the γγ jj final state in pp
             collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {782},
   Pages = {750-767},
   Year = {2018},
   Month = {July},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.06.011},
   Abstract = {This Letter presents a search for exotic decays of the Higgs
             boson to a pair of new (pseudo)scalar particles, H→aa,
             where the a particle has a mass in the range 20–60 GeV,
             and where one of the a bosons decays into a pair of photons
             and the other to a pair of gluons. The search is performed
             in event samples enhanced in vector-boson fusion Higgs boson
             production by requiring two jets with large invariant mass
             in addition to the Higgs boson candidate decay products. The
             analysis is based on the full dataset of pp collisions at
             s=13TeV recorded in 2015 and 2016 with the ATLAS detector at
             the CERN Large Hadron Collider, corresponding to an
             integrated luminosity of 36.7 fb−1. The data are in
             agreement with the Standard Model predictions and an upper
             limit at the 95% confidence level is placed on the
             production cross section times the branching ratio for the
             decay H→aa→γγgg. This limit ranges from 3.1 pb to 9.0
             pb depending on the mass of the a boson.},
   Doi = {10.1016/j.physletb.2018.06.011},
   Key = {fds356674}
}

@article{fds356535,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
             L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
             JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
             JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
             VA},
   Title = {Search for Higgs boson decays into two new low-mass spin-0
             particles in the 4b channel with the ATLAS detector using pp
             collisions at √s = 13 TeV},
   Journal = {Physical Review D},
   Volume = {102},
   Number = {11},
   Year = {2020},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.102.112006},
   Abstract = {This paper describes a search for beyond the Standard Model
             decays of the Higgs boson into a pair of new spin-0
             particles subsequently decaying into b-quark pairs, H → aa
             → (bb¯)(bb¯), using protonproton collision data
             collected by the ATLAS detector at the Large Hadron Collider
             at center-of-mass energy √s = 13 TeV. This search focuses
             on the range 15 GeV ≤ ma ≤ 30 GeV, where the decay
             products are collimated; it is complementary to a previous
             search in the same final state targeting the range 20 GeV
             ≤ ma ≤ 60 GeV, where the decay products are well
             separated. A novel strategy for the identification of the a
             → bb¯ decays is deployed to enhance the efficiency for
             topologies with small separation angles. The search is
             performed with 36 fb-1 of integrated luminosity collected in
             2015 and 2016 and sets upper limits on the production cross
             section of H → aa → (bb¯)(bb¯), where the Higgs boson
             is produced in association with a Z boson.},
   Doi = {10.1103/PhysRevD.102.112006},
   Key = {fds356535}
}

@article{fds307537,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and A°kesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ},
   Title = {Search for Higgs boson decays to a photon and a Z boson in
             pp collisions at s=7 and 8 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {732},
   Pages = {8-27},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.03.015},
   Abstract = {A search is reported for a neutral Higgs boson in the decay
             channel H→Zγ, Z→ℓ +ℓ -(ℓ = e, μ), using 4.5
             fb-1of pp collisions at s=7 TeV and 20.3 fb-1of pp
             collisions at s=8 TeV, recorded by the ATLAS detector at the
             CERN Large Hadron Collider. The observed distribution of the
             invariant mass of the three final-state particles,mℓℓγ,
             is consistent with the Standard Model hypothesis in the
             investigated mass range of 120-150 GeV. For a Higgs boson
             with a mass of 125.5 GeV, the observed upper limit at the
             95% confidence level is 11 times the Standard Model
             expectation. Upper limits are set on the cross section times
             branching ratio of a neutral Higgs boson with mass in the
             range 120-150 GeV between 0.13 and 0.5 pb for s=8 TeV at 95%
             confidence level. © 2014.},
   Doi = {10.1016/j.physletb.2014.03.015},
   Key = {fds307537}
}

@article{fds336453,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for Higgs boson decays to beyond-the-Standard-Model
             light bosons in four-lepton events with the ATLAS detector
             at √s=13 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2018},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2018)166},
   Abstract = {A search is conducted for a beyond-the-Standard-Model boson
             using events where a Higgs boson with mass 125 GeV decays to
             four leptons (ℓ = e or μ). This decay is presumed to
             occur via an intermediate state which contains one or two
             on-shell, promptly decaying bosons: H → ZX/XX → 4ℓ,
             where X is a new vector boson Zd or pseudoscalar a with mass
             between 1 and 60 GeV. The search uses pp collision data
             collected with the ATLAS detector at the LHC with an
             integrated luminosity of 36.1 fb−1 at a centre-of-mass
             energy s=13 TeV. No significant excess of events above
             Standard Model background predictions is observed;
             therefore, upper limits at 95% confidence level are set on
             modelindependent fiducial cross-sections, and on the Higgs
             boson decay branching ratios to vector and pseudoscalar
             bosons in two benchmark models.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP06(2018)166},
   Key = {fds336453}
}

@article{fds371449,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
             A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
             W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
             MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
   Title = {Search for Higgs boson pair production in association with a
             vector boson in pp collisions at √s=13TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {6},
   Year = {2023},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11559-y},
   Abstract = {This paper reports a search for Higgs boson pair (hh)
             production in association with a vector boson (WorZ) using
             139 fb - 1 of proton–proton collision data at s=13TeV
             recorded with the ATLAS detector at the Large Hadron
             Collider. The search is performed in final states in which
             the vector boson decays leptonically (W→ℓν,Z→ℓℓ,νν
             with ℓ= e, μ) and the Higgs bosons each decay into a pair
             of b-quarks. It targets Vhh signals from both non-resonant
             hh production, present in the Standard Model (SM), and
             resonant hh production, as predicted in some SM extensions.
             A 95% confidence-level upper limit of 183 (87) times the SM
             cross-section is observed (expected) for non-resonant Vhh
             production when assuming the kinematics are as expected in
             the SM. Constraints are also placed on Higgs boson coupling
             modifiers. For the resonant search, upper limits on the
             production cross-sections are derived for two specific
             models: one is the production of a vector boson along with a
             neutral heavy scalar resonance H, in the mass range
             260–1000 GeV, that decays into hh, and the other is the
             production of a heavier neutral pseudoscalar resonance A
             that decays into a Z boson and H boson, where the A boson
             mass is 360–800 GeV and the H boson mass is
             260–400 GeV. Constraints are also derived in the
             parameter space of two-Higgs-doublet models.},
   Doi = {10.1140/epjc/s10052-023-11559-y},
   Key = {fds371449}
}

@article{fds356615,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S},
   Title = {Search for Higgs boson pair production in the bb¯ WW
             * decay mode at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {4},
   Year = {2019},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2019)092},
   Abstract = {A search for Higgs boson pair production in the bb¯ WW *
             decay mode is performed in the bb¯ ℓνqq final state
             using 36.1 fb −1 of proton-proton collision data at a
             centre-of-mass energy of 13 TeV recorded with the ATLAS
             detector at the Large Hadron Collider. No evidence of events
             beyond the background expectation is found. Upper limits on
             the non-resonant pp → HH production cross section of 10 pb
             and on the resonant production cross section as a function
             of the HH invariant mass are obtained. Resonant production
             limits are set for scalar and spin-2 graviton hypotheses in
             the mass range 500 to 3000 GeV.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP04(2019)092},
   Key = {fds356615}
}

@article{fds356606,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {Search for Higgs boson pair production in the
             WW(*)WW(*) decay channel using ATLAS
             data recorded at √s = 13 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {5},
   Year = {2019},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2019)124},
   Abstract = {A search for a pair of neutral, scalar bosons with each
             decaying into two W bosons is presented using 36.1 fb−1 of
             proton-proton collision data at a centre-of-mass energy of
             13 TeV recorded with the ATLAS detector at the Large Hadron
             Collider. This search uses three production models:
             non-resonant and resonant Higgs boson pair production and
             resonant production of a pair of heavy scalar particles.
             Three final states, classified by the number of leptons, are
             analysed: two same-sign leptons, three leptons, and four
             leptons. No significant excess over the expected Standard
             Model backgrounds is observed. An observed (expected) 95%
             confidence-level upper limit of 160 (120) times the Standard
             Model prediction of non-resonant Higgs boson pair production
             cross-section is set from a combined analysis of the three
             final states. Upper limits are set on the production
             cross-section times branching ratio of a heavy scalar X
             decaying into a Higgs boson pair in the mass range of 260
             GeV ≤ mX ≤ 500 GeV and the observed (expected) limits
             range from 9.3 (10) pb to 2.8 (2.6) pb. Upper limits are set
             on the production cross-section times branching ratio of a
             heavy scalar X decaying into a pair of heavy scalars S for
             mass ranges of 280 GeV ≤ mX ≤ 340 GeV and 135 GeV ≤ mS
             ≤ 165 GeV and the observed (expected) limits range from
             2.5 (2.5) pb to 0.16 (0.17) pb.},
   Doi = {10.1007/JHEP05(2019)124},
   Key = {fds356606}
}

@article{fds321139,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH},
   Title = {Search for Higgs boson pair production in the [Formula: see
             text] final state from pp collisions at [Formula: see
             text] TeVwith the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {9},
   Pages = {412},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3628-x},
   Abstract = {A search for Higgs boson pair production [Formula: see text]
             is performed with 19.5 fb[Formula: see text] of
             proton-proton collision data at [Formula: see text] TeV,
             which were recorded by the ATLAS detector at the Large
             Hadron Collider in 2012. The decay products of each Higgs
             boson are reconstructed as a high-momentum [Formula: see
             text] system with either a pair of small-radius jets or a
             single large-radius jet, the latter exploiting jet
             substructure techniques and associated <i>b</i>-tagged
             track-jets. No evidence for resonant or non-resonant Higgs
             boson pair production is observed. The data are interpreted
             in the context of the Randall-Sundrum model with a warped
             extra dimension as well as the two-Higgs-doublet model. An
             upper limit on the cross-section for [Formula: see text] of
             3.2 (2.3) fb is set for a Kaluza-Klein graviton [Formula:
             see text] mass of 1.0 (1.5) TeV, at the 95 % confidence
             level. The search for non-resonant Standard Model <i>hh</i>
             production sets an observed 95 % confidence level upper
             limit on the production cross-section [Formula: see text] of
             202 fb, compared to a Standard Model prediction of
             [Formula: see text] fb.},
   Doi = {10.1140/epjc/s10052-015-3628-x},
   Key = {fds321139}
}

@article{fds356647,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Search for Higgs boson pair production in the γ γ bb¯
             final state with 13 TeV pp collision data collected by the
             ATLAS experiment},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {11},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2018)040},
   Abstract = {A search is performed for resonant and non-resonant Higgs
             boson pair production in the γ γ bb¯ final state. The
             data set used corresponds to an integrated luminosity of
             36.1 fb−1 of proton-proton collisions at a centre-of-mass
             energy of 13 TeV recorded by the ATLAS detector at the CERN
             Large Hadron Collider. No significant excess relative to the
             Standard Model expectation is observed. The observed limit
             on the non-resonant Higgs boson pair cross-section is 0.73
             pb at 95% confidence level. This observed limit is
             equivalent to 22 times the predicted Standard Model
             cross-section. The Higgs boson self-coupling (κλ =
             λHHH/λHHHSM) is constrained at 95% confidence level to
             −8.2 < κλ < 13.2. For resonant Higgs boson pair
             production through X→ HH→ γ γ bb¯ , the limit is
             presented, using the narrow-width approximation, as a
             function of mX in the range 260 GeV < mX < 1000 GeV. The
             observed limits range from 1.1 pb to 0.12 pb over this mass
             range.},
   Doi = {10.1007/JHEP11(2018)040},
   Key = {fds356647}
}

@article{fds347486,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Pereira, RA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines,
             JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Gupta, DB and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
             E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
             M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
             PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch,
             TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
             BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
             S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen, H and Chen, J and Chen,
             S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng,
             HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ},
   Title = {Search for Higgs boson pair production in the γ γ W W ∗
             channel using pp collision data recorded at s = 13 TeV with
             the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {12},
   Pages = {1007},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-6457-x},
   Abstract = {Searches for non-resonant and resonant Higgs boson pair
             production are performed in the γ γ W W ∗ channel with
             the final state of γ γ ℓ ν j j using 36.1  fb - 1 of
             proton-proton collision data recorded at a centre-of-mass
             energy of s = 13 TeV by the ATLAS detector at the Large
             Hadron Collider. No significant deviation from the Standard
             Model prediction is observed. A 95% confidence-level
             observed upper limit of 7.7 pb is set on the cross section
             for non-resonant production, while the expected limit is 5.4
             pb. A search for a narrow-width resonance <i>X</i> decaying
             to a pair of Standard Model Higgs bosons <i>HH</i> is
             performed with the same set of data, and the observed upper
             limits on σ ( p p → X ) × B ( X → H H ) range between
             40.0 and 6.1 pb for masses of the resonance between 260 and
             500 GeV, while the expected limits range between 17.6 and
             4.4 pb. When deriving the limits above, the Standard Model
             branching ratios of the H → γ γ and H → W W ∗ are
             assumed.},
   Doi = {10.1140/epjc/s10052-018-6457-x},
   Key = {fds347486}
}

@article{fds310302,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, M and Battistin,
             M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, MF and Besson, N and Betancourt,
             C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
             M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
             CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea,
             V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov,
             A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
             JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
             S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG},
   Title = {Search for Higgs boson pair production in the γγbb[over
             ¯] final state using pp collision data at
             sqrt[s]=8  TeV from the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {8},
   Pages = {081802},
   Year = {2015},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.114.081802},
   Abstract = {Searches are performed for resonant and nonresonant Higgs
             boson pair production in the γγbb[over ¯] final state
             using 20  fb^{-1} of proton-proton collisions at a
             center-of-mass energy of 8 TeV recorded with the ATLAS
             detector at the CERN Large Hadron Collider. A 95% confidence
             level upper limit on the cross section times branching ratio
             of nonresonant production is set at 2.2 pb, while the
             expected limit is 1.0 pb. The difference derives from a
             modest excess of events, corresponding to 2.4 standard
             deviations from the background-only hypothesis. The limit
             observed in the search for a narrow X→hh resonance ranges
             between 0.7 and 3.5 pb as a function of the resonance
             mass.},
   Doi = {10.1103/physrevlett.114.081802},
   Key = {fds310302}
}

@article{fds355955,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
             JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
             V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arguin,
             JF},
   Title = {Search for Higgs boson production in association with a
             high-energy photon via vector-boson fusion with decay into
             bottom quark pairs at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {3},
   Year = {2021},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2021)268},
   Abstract = {A search is presented for the production of the Standard
             Model Higgs boson in association with a high-energy photon.
             With a focus on the vector-boson fusion process and the
             dominant Higgs boson decay into b-quark pairs, the search
             benefits from a large reduction of multijet background
             compared to more inclusive searches. Results are reported
             from the analysis of 132 fb−1 of pp collision data at s =
             13 TeV collected with the ATLAS detector at the LHC. The
             measured Higgs boson signal yield in this final-state
             signature is 1.3 ± 1.0 times the Standard Model prediction.
             The observed significance of the Higgs boson signal above
             the background is 1.3 standard deviations, compared to an
             expected significance of 1.0 standard deviations. [Figure
             not available: see fulltext.]},
   Doi = {10.1007/JHEP03(2021)268},
   Key = {fds355955}
}

@article{fds362571,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
             JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
             V and Arcangeletti, C},
   Title = {Search for Higgs bosons decaying into new spin-0 or spin-1
             particles in four-lepton final states with the ATLAS
             detector with 139 fb −1 of pp collision data at
             √s = 13 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2022},
   Number = {3},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2022},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2022)041},
   Abstract = {Searches are conducted for new spin-0 or spin-1 bosons using
             events where a Higgs boson with mass 125 GeV decays into
             four leptons (ℓ = e, μ). This decay is presumed to occur
             via an intermediate state which contains two on-shell,
             promptly decaying bosons: H → XX/ZX → 4ℓ, where the
             new boson X has a mass between 1 and 60 GeV. The search uses
             pp collision data collected with the ATLAS detector at the
             LHC with an integrated luminosity of 139 fb−1 at a
             centre-of-mass energy s = 13 TeV. The data are found to be
             consistent with Standard Model expectations. Limits are set
             on fiducial cross sections and on the branching ratio of the
             Higgs boson to decay into XX/ZX, improving those from
             previous publications by a factor between two and four.
             Limits are also set on mixing parameters relevant in
             extensions of the Standard Model containing a dark sector
             where X is interpreted to be a dark boson. [Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP03(2022)041},
   Key = {fds362571}
}

@article{fds321136,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and T. H.
             Arce and A and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for higgs bosons decaying to aa in the µµττ final
             state in pp collisions at √s = 8 TeV with the ATLAS
             experiment},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {5},
   Pages = {052002-1-052002-24},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.052002},
   Abstract = {A search for the decay to a pair of new particles of either
             the 125 GeV Higgs boson (h) or a second charge parity
             (CP)-even Higgs boson (H) is presented. The data set
             corresponds to an integrated luminosity of 20.3 fb-1 of pp
             collisions at √s = 8 TeV recorded by the ATLAS experiment
             at the LHC in 2012. The search was done in the context of
             the next-to-minimal supersymmetric standard model, in which
             the new particles are the lightest neutral pseudoscalar
             Higgs bosons (a). One of the two a bosons is required to
             decay to two muons while the other is required to decay to
             two τ leptons. No significant excess is observed above the
             expected backgrounds in the dimuon invariant mass range from
             3.7 to 50 GeV. Upper limits are placed on the production of
             h → aa relative to the standard model gg → h production,
             assuming no coupling of the a boson to quarks. The most
             stringent limit is placed at 3.5% for ma = 3.75 GeV. Upper
             limits are also placed on the production cross section of H
             → aa from 2.33 to 0.72 pb, for fixed ma = 5 GeV with mH
             ranging from 100 to 500 GeV.},
   Doi = {10.1103/PhysRevD.92.052002},
   Key = {fds321136}
}

@article{fds308101,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, J-F and Arisawa, T and Artikov, A and Ashmanskas, W and Attal,
             A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
             J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
             J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Connolly, A and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cruz, A and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'onofrio, M and Dagenhart, D and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and Dell'Orso, M and Demers, S and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann, JR and DiTuro,
             P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers,
             J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
             M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
             LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia, JE and Garcia Sciverez and M and Garfinkel, AF and Gay, C and Gerberich, H and Gerchtein, E and Gerdes, D and Giagu, S and di
             Giovanni, GP and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
             C and Giokaris, N and Giolo, K and Giordani, M and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher,
             C and Grundler, U and Guimaraes da Costa and J and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
             RM and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heijboer,
             A and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang,
             D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karagoz-Unel,
             M and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Kordas, K and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreps, M and Kreymer, A and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen,
             AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev,
             DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca,
             G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin,
             M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, P and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
             A and von der Mey, M and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr,
             B and Moore, R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa,
             T and Oh, SH and Oh, YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Papikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pitts, K and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
             A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and van Remortel, N and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Rinnert, K and Ristori, L and Robertson,
             WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Salto, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle,
             T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria,
             F},
   Title = {Search for Higgs bosons decaying to bb and produced in
             association with W bosons in pp collisions at square root of
             s = 1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {96},
   Number = {8},
   Pages = {081803},
   Year = {2006},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.96.081803},
   Abstract = {We present a search for Higgs bosons decaying into bb and
             produced in association with W bosons in pp collisions at
             square root of s = 1.96 TeV. This search uses 320 pb(-1) of
             the data set accumulated by the upgraded Collider Detector
             at Fermilab. Events are selected that have a high-transverse
             momentum electron or muon, missing transverse energy, and
             two jets, at least one of which is consistent with the
             hadronization of a b quark. Both the number of events and
             the dijet mass distribution are consistent with standard
             model background expectations, and we set 95% confidence
             level upper limits on the production cross section times
             branching ratio for the Higgs boson or any new particle with
             similar decay kinematics. These upper limits range from 10
             pb for mH = 110 GeV/c2 to 3 pb for mH = 150
             GeV/c2.},
   Doi = {10.1103/physrevlett.96.081803},
   Key = {fds308101}
}

@article{fds307937,
   Author = {Aaltonen, T and others},
   Title = {Search for Higgs Bosons Predicted in Two-Higgs-Doublet
             Models via Decays to Tau Lepton Pairs in 1.96 TeV pp̅
             Collisions},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {20},
   Pages = {201801},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.201801},
   Abstract = {We present the results of a search for Higgs bosons
             predicted in two-Higgs-doublet models, in the case where the
             Higgs bosons decay to tau lepton pairs, using 1.8  fb-1
             of integrated luminosity of pp̅ collisions recorded by the
             CDF II experiment at the Fermilab Tevatron. Studying the
             mass distribution in events where one or both tau leptons
             decay leptonically, no evidence for a Higgs boson signal is
             observed. The result is used to infer exclusion limits in
             the two-dimensional space of tan⁡β versus mA (the ratio
             of the vacuum expectation values of the two Higgs doublets
             and the mass of the pseudoscalar boson, respectively).},
   Doi = {10.1103/physrevlett.103.201801},
   Key = {fds307937}
}

@article{fds307815,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D},
   Title = {Search for Higgs bosons produced in association with b
             quarks},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.032005},
   Abstract = {We present a search for neutral Higgs bosons decaying into
             bb̄, produced in association with b quarks in pp̄
             collisions. This process could be observable in
             supersymmetric models with high values of tanβ. The event
             sample corresponds to 2.6fb -1 of integrated luminosity
             collected with the CDF II detector at the Fermilab Tevatron
             collider. We search for an enhancement in the mass of the
             two leading jets in events with three jets identified as
             coming from b quarks using a displaced vertex algorithm. A
             data-driven procedure is used to estimate the dijet mass
             spectrum of the nonresonant multijet background. The
             contributions of backgrounds and a possible Higgs boson
             signal are determined by a two-dimensional fit of the data,
             using the dijet mass together with an additional variable
             which is sensitive to the flavor composition of the three
             tagged jets. We set mass-dependent limits on
             σ(pp̄→)×B(→bb̄) which are applicable for a narrow
             scalar particle produced in association with b quarks. We
             also set limits on tanβ in supersymmetric Higgs models
             including the effects of the Higgs boson width. © 2012
             American Physical Society.},
   Doi = {10.1103/PhysRevD.85.032005},
   Key = {fds307815}
}

@article{fds356663,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Search for Higgs bosons produced via vector-boson fusion and
             decaying into bottom quark pairs in s =13 TeV pp collisions
             with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {5},
   Year = {2018},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.052003},
   Abstract = {A search for the bb decay of the Standard Model Higgs boson
             produced through vector-boson fusion is presented. Three
             mutually exclusive channels are considered: two all-hadronic
             channels and a photon-associated channel. Results are
             reported from the analysis of up to 30.6 fb-1 of pp data at
             s=13 TeV collected with the ATLAS detector at the LHC. The
             measured signal strength relative to the Standard Model
             prediction from the combined analysis is 2.5-1.3+1.4 for
             inclusive Higgs boson production and 3.0-1.6+1.7 for
             vector-boson fusion production only.},
   Doi = {10.1103/PhysRevD.98.052003},
   Key = {fds356663}
}

@article{fds356619,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Search for Higgs-like particles produced in association with
             bottom quarks in proton-antiproton collisions},
   Journal = {Physical Review D},
   Volume = {99},
   Number = {5},
   Year = {2019},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.99.052001},
   Abstract = {We report on a search for a spin-zero non-standard model
             particle in proton-antiproton collisions collected by the
             Collider Detector at Fermilab at a center-of-mass-energy of
             1.96 TeV. This particle, the φ boson, is expected to decay
             into a bottom-antibottom quark pair and to be produced in
             association with at least one bottom quark. The data sample
             consists of events with three jets identified as initiated
             by bottom quarks and corresponds to 5.4 fb-1 of integrated
             luminosity. In each event, the invariant mass of the two
             most energetic jets is studied by looking for deviations
             from the multijet background, which is modeled using data.
             No evidence is found for such a particle. Exclusion upper
             limits ranging from 20 to 2 pb are set for the product of
             production cross sections times branching fraction for the
             hypothetical φ boson with mass between 100 and 300 GeV/c2.
             These are the most stringent constraints to
             date.},
   Doi = {10.1103/PhysRevD.99.052001},
   Key = {fds356619}
}

@article{fds307867,
   Author = {Collaboration, AVKWGAEAATLAS},
   Title = {Search for high mass dilepton resonances in pp collisions at
             7 TeV with the ATLAS experiment},
   Journal = {Physics Letters B},
   Volume = {700},
   Number = {3-4},
   Pages = {163-180},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.04.044},
   Abstract = {This Letter presents a search for high mass e+e- or μ+μ-
             resonances in pp collisions at √s=7 TeV at the LHC. The
             data were recorded by the ATLAS experiment during 2010 and
             correspond to a total integrated luminosity of ~40 pb-1. No
             statistically significant excess above the Standard Model
             expectation is observed in the search region of dilepton
             invariant mass above 110 GeV. Upper limits at the 95%
             confidence level are set on the cross section times
             branching ratio of Z' resonances decaying to dielectrons and
             dimuons as a function of the resonance mass. A lower mass
             limit of 1.048 TeV on the Sequential Standard Model Z' boson
             is derived, as well as mass limits on Z* and E6-motivated Z'
             models. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.04.044},
   Key = {fds307867}
}

@article{fds307853,
   Author = {Collaboration, AVKWTAEACDF},
   Title = {Search for High Mass Resonances Decaying to Muon Pairs in
             √s=1.96  TeV pp̅ Collisions},
   Journal = {Physical Review Letters},
   Volume = {106},
   Number = {121801},
   Pages = {7},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.121801},
   Abstract = {We present a search for a new narrow, spin-1, high mass
             resonance decaying to μ(+)μ⁻+X, using a
             matrix-element-based likelihood and a simultaneous
             measurement of the resonance mass and production rate. In
             data with 4.6 fb⁻¹ of integrated luminosity collected by
             the CDF detector in pp collisions at √s=1960 GeV, the most
             likely signal cross section is consistent with zero at 16%
             confidence level. We therefore do not observe evidence for a
             high mass resonance and place limits on models predicting
             spin-1 resonances, including M>1071 GeV/c² at 95%
             confidence level for a Z' boson with the same couplings to
             fermions as the Z boson.},
   Doi = {10.1103/PhysRevLett.106.121801},
   Key = {fds307853}
}

@article{fds313612,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
             G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for high-mass diboson resonances with boson-tagged
             jets in proton-proton collisions at √s = 8TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {12},
   Pages = {1-39},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2015)055},
   Abstract = {Abstract: A search is performed for narrow resonances
             decaying into WW, WZ, or ZZ boson pairs using 20.3 fb−1 of
             proton-proton collision data at a centre-of-mass energy of
             s=8$$ \sqrt{s}=8 $$ TeV recorded with the ATLAS detector at
             the Large Hadron Collider. Diboson resonances with masses in
             the range from 1.3 to 3.0 TeV are sought after using the
             invariant mass distribution of dijets where both jets are
             tagged as a boson jet, compatible with a highly boosted W or
             Z boson decaying to quarks, using jet mass and substructure
             properties. The largest deviation from a smoothly falling
             background in the observed dijet invariant mass distribution
             occurs around 2 TeV in the WZ channel, with a global
             significance of 2.5 standard deviations. Exclusion limits at
             the 95% confidence level are set on the production cross
             section times branching ratio for the WZ final state of a
             new heavy gauge boson, W′, and for the WW and ZZ final
             states of Kaluza-Klein excitations of the graviton in a bulk
             Randall-Sundrum model, as a function of the resonance mass.
             W′ bosons with couplings predicted by the extended gauge
             model in the mass range from 1.3 to 1.5 TeV are excluded at
             95% confidence level.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP12(2015)055},
   Key = {fds313612}
}

@article{fds310363,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allen, K and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O},
   Title = {Search for high-mass dilepton resonances in pp collisions at
             s =8 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {September},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.052005},
   Abstract = {The ATLAS detector at the Large Hadron Collider is used to
             search for high-mass resonances decaying to dielectron or
             dimuon final states. Results are presented from an analysis
             of proton-proton (pp) collisions at a center-of-mass energy
             of 8 TeV corresponding to an integrated luminosity of 20.3
             fb-1 in the dimuon channel. A narrow resonance with Standard
             Model Z couplings to fermions is excluded at 95% confidence
             level for masses less than 2.79 TeV in the dielectron
             channel, 2.53 TeV in the dimuon channel, and 2.90 TeV in the
             two channels combined. Limits on other model interpretations
             are also presented, including a grand-unification model
             based on the E6 gauge group, Z∗ bosons, minimal Z′
             models, a spin-2 graviton excitation from Randall-Sundrum
             models, quantum black holes, and a minimal walking
             technicolor model with a composite Higgs
             boson.},
   Doi = {10.1103/PhysRevD.90.052005},
   Key = {fds310363}
}

@article{fds356575,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP},
   Title = {Search for high-mass dilepton resonances using 139
             fb−1 of pp collision data collected at √s=13
             TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {796},
   Pages = {68-87},
   Year = {2019},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.07.016},
   Abstract = {A search for high-mass dielectron and dimuon resonances in
             the mass range of 250 GeV to 6 TeV is presented. The data
             were recorded by the ATLAS experiment in proton–proton
             collisions at a centre-of-mass energy of s=13 TeV during Run
             2 of the Large Hadron Collider and correspond to an
             integrated luminosity of 139 fb−1. A functional form is
             fitted to the dilepton invariant-mass distribution to model
             the contribution from background processes, and a generic
             signal shape is used to determine the significance of
             observed deviations from this background estimate. No
             significant deviation is observed and upper limits are
             placed at the 95% confidence level on the fiducial
             cross-section times branching ratio for various resonance
             width hypotheses. The derived limits are shown to be
             applicable to spin-0, spin-1 and spin-2 signal hypotheses.
             For a set of benchmark models, the limits are converted into
             lower limits on the resonance mass and reach 4.5 TeV for the
             E6-motivated Zψ′ boson. Also presented are limits on
             Heavy Vector Triplet model couplings.},
   Doi = {10.1016/j.physletb.2019.07.016},
   Key = {fds356575}
}

@article{fds310265,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for high-mass diphoton resonances in pp collisions at
             s =8 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.032004},
   Abstract = {This article describes a search for high-mass resonances
             decaying to a pair of photons using a sample of 20.3 fb-1 of
             pp collisions at s=8 TeV recorded with the ATLAS detector at
             the Large Hadron Collider. The data are found to be in
             agreement with the Standard Model prediction, and limits are
             reported in the framework of the Randall-Sundrum model. This
             theory leads to the prediction of graviton states, the
             lightest of which could be observed at the Large Hadron
             Collider. A lower limit of 2.66 (1.41) TeV at 95% confidence
             level is set on the mass of the lightest graviton for
             couplings of k/M¯Pl=0.1 (0.01).},
   Doi = {10.1103/PhysRevD.92.032004},
   Key = {fds310265}
}

@article{fds307963,
   Author = {Aaltonen, T and others},
   Title = {Search for High-Mass e+e- Resonances in ppbar Collisions at
             1.96 TeV},
   Journal = {PRL},
   Volume = {102},
   Number = {3},
   Pages = {031801},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.031801},
   Abstract = {A search for high-mass resonances in the e+e- final state is
             presented based on 2.5 fb(-1) of sqrt[s]=1.96 TeV pp
             collision data from the CDF II detector at the Fermilab
             Tevatron. The largest excess over the standard model
             prediction is at an e+e- invariant mass of 240 GeV/c2. The
             probability of observing such an excess arising from
             fluctuations in the standard model anywhere in the mass
             range of 150-1000 GeV/c2 is 0.6% (equivalent to 2.5sigma).
             We exclude the standard model coupling Z' and the
             Randall-Sundrum graviton for k/MPl=0.1 with masses below 963
             and 848 GeV/c2 at the 95% credibility level,
             respectively.},
   Doi = {10.1103/physrevlett.102.031801},
   Key = {fds307963}
}

@article{fds321081,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Search for high-mass new phenomena in the dilepton final
             state using proton–proton collisions at s=13TeV with the
             ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {761},
   Pages = {372-392},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.08.055},
   Abstract = {A search is conducted for both resonant and non-resonant
             high-mass new phenomena in dielectron and dimuon final
             states. The search uses 3.2fb−1 of proton–proton
             collision data, collected at s=13TeV by the ATLAS experiment
             at the LHC in 2015. The dilepton invariant mass is used as
             the discriminating variable. No significant deviation from
             the Standard Model prediction is observed; therefore limits
             are set on the signal model parameters of interest at 95%
             credibility level. Upper limits are set on the cross-section
             times branching ratio for resonances decaying to dileptons,
             and the limits are converted into lower limits on the
             resonance mass, ranging between 2.74 TeV and 3.36 TeV,
             depending on the model. Lower limits on the ℓℓqq contact
             interaction scale are set between 16.7 TeV and 25.2 TeV,
             also depending on the model.},
   Doi = {10.1016/j.physletb.2016.08.055},
   Key = {fds321081}
}

@article{fds313581,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'Errico, M},
   Title = {Search for high-mass resonances decaying into ZZ in pp̄
             collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   ISSN = {1550-7998},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000299925100002&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Abstract = {We search for high-mass resonances decaying into Z boson
             pairs using data corresponding to 6fb -1 collected by the
             CDF experiment in pp̄ collisions at √s=1.96TeV. The
             search is performed in three distinct final states: ZZ→
             +-+-, ZZ→ +-νν, and ZZ→ +-jj. For a Randall-Sundrum
             graviton G *, the 95% CL upper limits on the production
             cross section times branching ratio to ZZ, σ(pp̄→G
             *→ZZ), vary between 0.26 pb and 0.045 pb in the mass range
             300<M G*<1000GeV/c2. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.85.012008},
   Key = {fds313581}
}

@article{fds311114,
   Author = {Collaboration, AVKWATLAS},
   Title = {Search for high-mass resonances decaying to dilepton final
             states in pp collisions at √s = 7 TeV with the ATLAS
             detector},
   Journal = {JHEP},
   Volume = {11},
   Number = {11},
   Pages = {138},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2012)138},
   Abstract = {The ATLAS detector at the Large Hadron Collider is used to
             search for highmass resonances decaying to an
             electron-positron pair or a muon-antimuon pair. The search
             is sensitive to heavy neutral Z′ gauge bosons,
             Randall-Sundrum gravitons, Z* bosons, techni-mesons,
             Kaluza-Klein Z/γ bosons, and bosons predicted by Torsion
             models. Results are presented based on an analysis of pp
             collisions at a center-of-mass energy of 7 TeV corresponding
             to an integrated luminosity of 4.9 fb-1 in the e +e- channel
             and 5.0 fb-1 in the μ+μ- channel. A Z′ boson with
             Standard Model-like couplings is excluded at 95% confidence
             level for masses below 2.22 TeV. A Randall-Sundrum graviton
             with coupling k /M̄Pl = 0.1 is excluded at 95% confidence
             level for masses below 2.16 TeV. Limits on the other models
             are also presented, including Technicolor and Minimal Z′
             Models. Copyright CERN.},
   Doi = {10.1007/JHEP11(2012)138},
   Key = {fds311114}
}

@article{fds311279,
   Author = {al, AVKWTAE and Collaboration, CDF},
   Title = {Search for High-Mass Resonances Decaying to Dimuons at
             CDF},
   Journal = {Physical Review Letters},
   Volume = {102},
   Number = {091805},
   Pages = {6},
   Year = {2009},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.102.091805},
   Abstract = {We present a search for high-mass neutral resonances using
             dimuon data corresponding to an integrated luminosity of 2.3
             fb(-1) collected in pp[over ] collisions at sqrt[s]=1.96 TeV
             by the CDF II detector at the Fermilab Tevatron. No
             significant excess above the standard model expectation is
             observed in the dimuon invariant-mass spectrum. We set 95%
             confidence level upper limits on sigmaBR(pp-->X-->micromicro),
             where X is a boson with spin-0, 1, or 2. Using these cross
             section limits, we determine lower mass limits on sneutrinos
             in R-parity-violating supersymmetric models, Z' bosons, and
             Kaluza-Klein gravitons in the Randall-Sundrum
             model.},
   Doi = {10.1103/physrevlett.102.091805},
   Key = {fds311279}
}

@article{fds307960,
   Author = {Aaltonen, T and others},
   Title = {Search for High-Mass Resonances Decaying to Dimuons at
             CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {9},
   Pages = {091805},
   Publisher = {APS},
   Year = {2009},
   Month = {Spring},
   url = {http://dx.doi.org/10.1103/PhysRevLett.102.091805},
   Abstract = {We present a search for high-mass neutral resonances using
             dimuon data corresponding to an integrated luminosity of 2.3
             fb(-1) collected in pp[over ] collisions at sqrt[s]=1.96 TeV
             by the CDF II detector at the Fermilab Tevatron. No
             significant excess above the standard model expectation is
             observed in the dimuon invariant-mass spectrum. We set 95%
             confidence level upper limits on sigmaBR(pp-->X-->micromicro),
             where X is a boson with spin-0, 1, or 2. Using these cross
             section limits, we determine lower mass limits on sneutrinos
             in R-parity-violating supersymmetric models, Z' bosons, and
             Kaluza-Klein gravitons in the Randall-Sundrum
             model.},
   Doi = {10.1103/PhysRevLett.102.091805},
   Key = {fds307960}
}

@article{fds308093,
   Author = {Abulencia, and A, and others},
   Title = {Search for high-mass resonances decaying to e mu in
             $p\bar{p}$ collisions at $\sqrt{s} =$ 1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {21},
   Pages = {211802},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.211802},
   Abstract = {We describe a general search for resonances decaying to a
             neutral e mu final state in p anti-p collisions at a
             center-of-mass energy of 1.96 TeV. Using a data sample
             representing 344 pb-1 of integrated luminosity recorded by
             the CDF II experiment, we compare Standard Model predictions
             with the number of observed events for invariant masses
             between 50 and 800 GeV/c2. Finding no significant excess (5
             events observed vs. 7.7 +/- 0.8 expected for M_e mu > 100
             GeV/c2), we set limits on sneutrino and Z' masses as
             functions of lepton family number violating
             couplings.},
   Doi = {10.1103/physrevlett.96.211802},
   Key = {fds308093}
}

@article{fds347462,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJ and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov,
             A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
             G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
             Kuutmann, E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
             O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
             AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov,
             A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
             D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko,
             D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer,
             F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, J and Chen, S and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard,
             AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Clark, A and Clark, MR},
   Title = {Search for High-Mass Resonances Decaying to τν in pp
             Collisions at sqrt[s]=13  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {120},
   Number = {16},
   Pages = {161802},
   Year = {2018},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.120.161802},
   Abstract = {A search for high-mass resonances decaying to τν using
             proton-proton collisions at sqrt[s]=13  TeV produced by
             the Large Hadron Collider is presented. Only τ-lepton
             decays with hadrons in the final state are considered. The
             data were recorded with the ATLAS detector and correspond to
             an integrated luminosity of 36.1  fb^{-1}. No
             statistically significant excess above the standard model
             expectation is observed; model-independent upper limits are
             set on the visible τν production cross section. Heavy
             W^{'} bosons with masses less than 3.7 TeV in the
             sequential standard model and masses less than 2.2-3.8 TeV
             depending on the coupling in the nonuniversal G(221) model
             are excluded at the 95% credibility level.},
   Doi = {10.1103/physrevlett.120.161802},
   Key = {fds347462}
}

@article{fds310312,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H},
   Title = {Search for H→γγ produced in association with top quarks
             and constraints on the Yukawa coupling between the top quark
             and the Higgs boson using data taken at 7 TeV and 8 TeV with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {740},
   Pages = {222-242},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.11.049},
   Abstract = {A search is performed for Higgs bosons produced in
             association with top quarks using the diphoton decay mode of
             the Higgs boson. Selection requirements are optimized
             separately for leptonic and fully hadronic final states from
             the top quark decays. The dataset used corresponds to an
             integrated luminosity of 4.5 fb−1 of proton–proton
             collisions at a center-of-mass energy of 7 TeV and 20.3
             fb−1 at 8 TeV recorded by the ATLAS detector at the CERN
             Large Hadron Collider. No significant excess over the
             background prediction is observed and upper limits are set
             on the tt¯H production cross section. The observed
             exclusion upper limit at 95% confidence level is 6.7 times
             the predicted Standard Model cross section value. In
             addition, limits are set on the strength of the Yukawa
             coupling between the top quark and the Higgs boson, taking
             into account the dependence of the tt¯H and tH cross
             sections as well as the H→γγ branching fraction on the
             Yukawa coupling. Lower and upper limits at 95% confidence
             level are set at −1.3 and +8.0 times the Yukawa coupling
             strength in the Standard Model.},
   Doi = {10.1016/j.physletb.2014.11.049},
   Key = {fds310312}
}

@article{fds313584,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
             M},
   Title = {Search for invisible decays of a Higgs boson produced in
             association with a Z boson in ATLAS},
   Journal = {Physical Review Letters},
   Volume = {112},
   Number = {20},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {May},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.112.201802},
   Abstract = {A search for evidence of invisible-particle decay modes of a
             Higgs boson produced in association with a Z boson at the
             Large Hadron Collider is presented. No deviation from the
             standard model expectation is observed in 4.5 fb-1 (20.3
             fb-1) of 7 (8) TeV pp collision data collected by the ATLAS
             experiment. Assuming the standard model rate for ZH
             production, an upper limit of 75%, at the 95% confidence
             level is set on the branching ratio to invisible-particle
             decay modes of the Higgs boson at a mass of 125.5 GeV. The
             limit on the branching ratio is also interpreted in terms of
             an upper limit on the allowed dark matter-nucleon scattering
             cross section within a Higgs-portal dark matter scenario.
             Within the constraints of such a scenario, the results
             presented in this Letter provide the strongest available
             limits for low-mass dark matter candidates. Limits are also
             set on an additional neutral Higgs boson, in the mass range
             110 <mH <400 GeV, produced in association with a Z boson and
             decaying to invisible particles.},
   Doi = {10.1103/PhysRevLett.112.201802},
   Key = {fds313584}
}

@article{fds356784,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for invisible decays of a Higgs boson using
             vector-boson fusion in pp collisions at √s=8 TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {1},
   Pages = {1-44},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2016)172},
   Abstract = {A search for a Higgs boson produced via vector-boson fusion
             and decaying into invisible particles is presented, using
             20.3 fb−1of proton-proton collision data at a
             centre-of-mass energy of 8 TeV recorded by the ATLAS
             detector at the LHC. For a Higgs boson with a mass of 125
             GeV, assuming the Standard Model production cross section,
             an upper bound of 0.28 is set on the branching fraction of H
             → invisible at 95% confidence level, where the expected
             upper limit is 0.31. The results are interpreted in models
             of Higgs-portal dark matter where the branching fraction
             limit is converted into upper bounds on the
             dark-matter-nucleon scattering cross section as a function
             of the dark-matter particle mass, and compared to results
             from the direct dark-matter detection experiments.},
   Doi = {10.1007/JHEP01(2016)172},
   Key = {fds356784}
}

@article{fds310332,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA},
   Title = {Search for invisible decays of the Higgs boson produced in
             association with a hadronically decaying vector boson in
             pp collisions at [Formula: see text] TeV with the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {337},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3551-1},
   Abstract = {A search for Higgs boson decays to invisible particles is
             performed using 20.3 [Formula: see text] of <i>pp</i>
             collision data at a centre-of-mass energy of 8 TeV recorded
             by the ATLAS detector at the Large Hadron Collider. The
             process considered is Higgs boson production in association
             with a vector boson ([Formula: see text] or <i>Z</i>) that
             decays hadronically, resulting in events with two or more
             jets and large missing transverse momentum. No excess of
             candidates is observed in the data over the background
             expectation. The results are used to constrain <i>VH</i>
             production followed by <i>H</i> decaying to invisible
             particles for the Higgs boson mass range [Formula: see
             text] GeV. The 95 % confidence-level observed upper limit
             on [Formula: see text] varies from 1.6 pb at 115 GeV to
             0.13 pb at 300 GeV. Assuming Standard Model production and
             including the [Formula: see text] contribution as signal,
             the results also lead to an observed upper limit of 78 % at
             95 % confidence level on the branching ratio of Higgs
             bosons decays to invisible particles at a mass of
             125 GeV.},
   Doi = {10.1140/epjc/s10052-015-3551-1},
   Key = {fds310332}
}

@article{fds356589,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
             Pereira, R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H},
   Title = {Search for invisible Higgs boson decays in vector boson
             fusion at s=13TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {793},
   Pages = {499-519},
   Year = {2019},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.04.024},
   Abstract = {We report a search for Higgs bosons that are produced via
             vector boson fusion and subsequently decay into invisible
             particles. The experimental signature is an energetic jet
             pair with invariant mass of O(1)TeV and O(100)GeV missing
             transverse momentum. The analysis uses 36.1 fb−1 of pp
             collision data at s=13TeV recorded by the ATLAS detector at
             the LHC. In the signal region the 2252 observed events are
             consistent with the background estimation. Assuming a 125GeV
             scalar particle with Standard Model cross sections, the
             upper limit on the branching fraction of the Higgs boson
             decay into invisible particles is 0.37 at 95% confidence
             level where 0.28 was expected. This limit is interpreted in
             Higgs portal models to set bounds on the WIMP–nucleon
             scattering cross section. We also consider invisible decays
             of additional scalar bosons with masses up to 3TeV for which
             the upper limits on the cross section times branching
             fraction are in the range of 0.3–1.7pb.},
   Doi = {10.1016/j.physletb.2019.04.024},
   Key = {fds356589}
}

@article{fds310318,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos,
             G and Azuma, Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek,
             P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil,
             HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
             N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell,
             WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
             CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
             V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron,
             J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
             AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S},
   Title = {Search for invisible particles produced in association with
             single-top-quarks in proton-proton collisions at [Formula:
             see text] with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {2},
   Pages = {79},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3233-4},
   Abstract = {A search for the production of single-top-quarks in
             association with missing energy is performed in
             proton-proton collisions at a centre-of-mass energy of
             [Formula: see text] with the ATLAS experiment at the large
             hadron collider using data collected in 2012, corresponding
             to an integrated luminosity of [Formula: see
             text] fb[Formula: see text]. In this search, the [Formula:
             see text] boson from the top quark is required to decay into
             an electron or a muon and a neutrino. No deviation from the
             standard model prediction is observed, and upper limits are
             set on the production cross-section for resonant and
             non-resonant production of an invisible exotic state in
             association with a right-handed top quark. In the case of
             resonant production, for a spin-[Formula: see text]
             resonance with a mass of [Formula: see text] GeV, an
             effective coupling strength above [Formula: see text] is
             excluded at 95[Formula: see text] confidence level for the
             top quark and an invisible spin-[Formula: see text] state
             with mass between [Formula: see text] and [Formula: see
             text] GeV. In the case of non-resonant production, an
             effective coupling strength above [Formula: see text] is
             excluded at 95[Formula: see text] confidence level for the
             top quark and an invisible spin-[Formula: see text] state
             with mass between [Formula: see text] and [Formula: see
             text] GeV.},
   Doi = {10.1140/epjc/s10052-014-3233-4},
   Key = {fds310318}
}

@article{fds308183,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
             JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
             R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
             D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MA and Cutts, D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gibbard, B and Gilmartin, R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grudberg, P and Grünendahl, S and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hou, S and Huang, Y and Ito, AS and Jerger, SA and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Karmanov, D and Karmgard, D and Kehoe, R and Kim, SK and Klima, B and Klopfenstein, C and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kuznetsov, VE and Landsberg, G and Leflat, A and Lehner,
             F and Li, J and Li, QZ and Lima, JG and Lincoln, D and Linn, SL and Linnemann,
             J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Maciel,
             AK and Madaras, RJ and Manankov, V and Mao, HS and Marshall, T and Martin,
             MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy,
             R and McDonald, J and McMahon, T and Melanson, HL and Meng, XC and Merkin,
             M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea, D and Mincer,
             A and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery, HE and Moore,
             RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Norman, D and Oesch, L and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan,
             LJ and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno,
             M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Qian, J and Quintas, PZ and Raja, R and Rajagopalan,
             S and Ramberg, E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Schwartzman, A and Sculli, J and Sen, N and Shabalina,
             E and Shankar, HC and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell,
             RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery,
             P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stevenson, ML and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Streets, K and Strovink,
             M and Stutte, L and Sznajder, A and Taylor, W and Tentindo-Repond, S and Thompson, J and Toback, D and Tripathi, SM and Trippe, TG and Turcot,
             AS and Tuts, PM and van Gemmeren, P and Vaniev, V and Van Kooten and R and Varelas, N and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, Z and Warchol, J and Watts, G and Wayne, M and Weerts, H and White,
             A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Wirjawan, JV and Womersley, J and Wood,
             DR and Yamada, R and Yamin, P and Yasuda, T and Yip, K and Youssef, S and Yu,
             J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zhu, ZH and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev,
             EG and Zylberstejn, A},
   Title = {Search for large extra dimensions in dielectron and diphoton
             production.},
   Journal = {Physical review letters},
   Volume = {86},
   Number = {7},
   Pages = {1156-1161},
   Year = {2001},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.86.1156},
   Abstract = {We report a search for effects of large extra spatial
             dimensions in pp collisions at a center-of-mass energy of
             1.8 TeV with the D0 detector, using events containing a pair
             of electrons or photons. The data are in good agreement with
             the expected background and do not exhibit evidence for
             large extra dimensions. We set the most restrictive lower
             limits to date, at the 95% C.L. on the effective Planck
             scale between 1.0 and 1.4 TeV for several formalisms and
             numbers of extra dimensions.},
   Doi = {10.1103/physrevlett.86.1156},
   Key = {fds308183}
}

@article{fds308087,
   Author = {Abulencia, and A, and others},
   Title = {Search for large extra dimensions in the production of jets
             and missing transverse energy in $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {97},
   Number = {17},
   Pages = {171802},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.97.171802},
   Abstract = {We present the results of a search for new physics in the
             jets plus missing transverse energy data sample collected
             from 368 pb-1 of p anti-p collisions at s**(1/2) = 1.96 TeV
             recorded by the Collider Detector at Fermilab. We compare
             the number of events observed in the data with a data-based
             estimate of the standard model backgrounds contributing to
             this signature. We observe no significant excess of events,
             and we interpret this null result in terms of lower limits
             on the fundamental Planck scale for a large extra dimensions
             scenario.},
   Doi = {10.1103/physrevlett.97.171802},
   Key = {fds308087}
}

@article{fds356602,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster,
             AJ},
   Title = {Search for large missing transverse momentum in association
             with one top-quark in proton-proton collisions at √s = 13
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {5},
   Year = {2019},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2019)041},
   Abstract = {This paper describes a search for events with one top-quark
             and large missing transverse momentum in the final state.
             Data collected during 2015 and 2016 by the ATLAS experiment
             from 13 TeV proton–proton collisions at the LHC
             corresponding to an integrated luminosity of 36.1 fb −1
             are used. Two channels are considered, depending on the
             leptonic or the hadronic decays of the W boson from the top
             quark. The obtained results are interpreted in the context
             of simplified models for dark-matter production and for the
             single production of a vector-like T quark. In the absence
             of significant deviations from the Standard Model background
             expectation, 95% confidence-level upper limits on the
             corresponding production cross-sections are obtained and
             these limits are translated into constraints on the
             parameter space of the models considered.[Figure not
             available: see fulltext.].},
   Doi = {10.1007/JHEP05(2019)041},
   Key = {fds356602}
}

@article{fds356648,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
   Title = {Search for lepton-flavor violation in different-flavor,
             high-mass final states in pp collisions at s =13 TeV with
             the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {9},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.092008},
   Abstract = {A search is performed for a heavy particle decaying into
             different-flavor, dilepton pairs (eμ, eτ or μτ), using
             36.1 fb-1 of proton-proton collision data at s=13 TeV
             collected in 2015-2016 by the ATLAS detector at the Large
             Hadron Collider. No excesses over the Standard Model
             predictions are observed. Bayesian lower limits at the 95%
             credibility level are placed on the mass of a Z′ boson,
             the mass of a supersymmetric τ-sneutrino, and on the
             threshold mass for quantum black-hole production. For the
             Z′ and sneutrino models, upper cross-section limits are
             converted to upper limits on couplings, which are compared
             with similar limits from low-energy experiments and which
             are more stringent for the eτ and μτ modes.},
   Doi = {10.1103/PhysRevD.98.092008},
   Key = {fds356648}
}

@article{fds361985,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin,
             RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Austrup, VA and Avner, G and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Backman, F and Badea, A and Bagnaia, P and Bahrasemani, H and Bailey,
             AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker,
             PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian,
             R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Balunas,
             WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev,
             A and Basan, A and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
             M and Bauce, M and Bauer, F and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
             P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov,
             VA and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel,
             F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold,
             A and Bertram, IA and Bessidskaia Bylund and O and Bethke, S and Betti, A and Bevan, AJ and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler, S and Brickwedde,
             B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom,
             PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard,
             BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
             AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
             VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente
             Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero,
             J and Cao, Y and Capua, M and Carbone, A and Cardarelli, R and Cardillo, F and Carducci, G and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carratta, G and Carter, JWS and Carter, TM and Casadei,
             D and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
             DG and Charman, TP and Chatterjee, M and Chau, CC and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen,
             CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, CL and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, YS and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark,
             A and Clark, PJ and Clavijo Columbie and JM and Clawson, SE and Clement,
             C},
   Title = {Search for Lepton-Flavor Violation in Z-Boson Decays with τ
             Leptons with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {127},
   Number = {27},
   Pages = {271801},
   Year = {2021},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.127.271801},
   Abstract = {A search for lepton-flavor-violating Z→eτ and Z→μτ
             decays with pp collision data recorded by the ATLAS detector
             at the LHC is presented. This analysis uses 139  fb^{-1}
             of Run 2 pp collisions at sqrt[s]=13  TeV and is
             combined with the results of a similar ATLAS search in the
             final state in which the τ lepton decays hadronically,
             using the same data set as well as Run 1 data. The addition
             of leptonically decaying τ leptons significantly improves
             the sensitivity reach for Z→ℓτ decays. The Z→ℓτ
             branching fractions are constrained in this analysis to
             B(Z→eτ)<7.0×10^{-6} and B(Z→μτ)<7.2×10^{-6} at 95%
             confidence level. The combination with the previously
             published analyses sets the strongest constraints to date:
             B(Z→eτ)<5.0×10^{-6} and B(Z→μτ)<6.5×10^{-6} at 95%
             confidence level.},
   Doi = {10.1103/physrevlett.127.271801},
   Key = {fds361985}
}

@article{fds356649,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
   Title = {Search for lepton-flavor-violating decays of the Z boson
             into a τ lepton and a light lepton with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {9},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.092010},
   Abstract = {Direct searches for lepton flavor violation in decays of the
             Z boson with the ATLAS detector at the LHC are presented.
             Decays of the Z boson into an electron or muon and a
             hadronically decaying τ lepton are considered. The searches
             are based on a data sample of proton-proton collisions
             collected by the ATLAS detector in 2015 and 2016,
             corresponding to an integrated luminosity of 36.1 fb-1 at a
             center-of-mass energy of s=13 TeV. No statistically
             significant excess of events above the expected background
             is observed, and upper limits on the branching ratios of
             lepton-flavor-violating decays are set at the 95% confidence
             level: B(Z→eτ)<5.8×10-5 and B(Z→μτ)<2.4×10-5. This
             is the first limit on B(Z→eτ) with ATLAS data. The upper
             limit on B(Z→μτ) is combined with a previous ATLAS
             result based on 20.3 fb-1 of proton-proton collision data at
             a center-of-mass energy of s=8 TeV and the combined upper
             limit at 95% confidence level is B(Z→μτ)<1.3×10-5.},
   Doi = {10.1103/PhysRevD.98.092010},
   Key = {fds356649}
}

@article{fds347491,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
             K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard,
             J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán,
             SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura,
             P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana,
             S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
             E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito,
             L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont,
             AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Search for lepton-flavour-violating decays of the Higgs and
             Z bosons with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {2},
   Pages = {70},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4624-0},
   Abstract = {Direct searches for lepton flavour violation in decays of
             the Higgs and <i>Z</i> bosons with the ATLAS detector at the
             LHC are presented. The following three decays are
             considered: [Formula: see text], [Formula: see text], and
             [Formula: see text]. The searches are based on the data
             sample of proton-proton collisions collected by the ATLAS
             detector corresponding to an integrated luminosity of
             20.3 [Formula: see text] at a centre-of-mass energy of
             [Formula: see text] TeV. No significant excess is observed,
             and upper limits on the lepton-flavour-violating branching
             ratios are set at the 95[Formula: see text] confidence
             level: Br[Formula: see text], Br[Formula: see text], and
             Br[Formula: see text].},
   Doi = {10.1140/epjc/s10052-017-4624-0},
   Key = {fds347491}
}

@article{fds348987,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for lepton-flavour-violating H → μτ decays of the
             Higgs boson with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {11},
   Pages = {1-33},
   Year = {2015},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2015)211},
   Abstract = {A direct search for lepton-flavour-violating H → μτ
             decays of the recently discovered Higgs boson with the ATLAS
             detector at the LHC is presented. The analysis is performed
             in the H → μτhad channel, where τhad is a hadronically
             decaying τ -lepton. The search is based on the data sample
             of proton-proton collisions collected by the ATLAS
             experiment corresponding to an integrated luminosity of 20.3
             fb−1 at a centre-of-mass energy of TeV. No statistically
             significant excess of data over the predicted background is
             observed. The observed (expected) 95% confidence-level upper
             limit on the branching fraction, Br(H → μτ ), is 1.85%
             (1.24%).[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP11(2015)211},
   Key = {fds348987}
}

@article{fds308173,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon,
             TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
             VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
             F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko,
             LV},
   Title = {Search for Leptoquark Pairs Decaying into [Formula
             presented] in [Formula presented] Collisions at [Formula
             presented]},
   Journal = {Physical Review Letters},
   Volume = {88},
   Number = {19},
   Pages = {7},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.88.191801},
   Abstract = {We present the results of a search for leptoquark (LQ) pairs
             in [Formula presented] of [Formula presented] collider data
             collected by the D0 experiment at the Fermilab Tevatron. We
             observe no evidence for leptoquark production and set a
             limit on [Formula presented] as a function of the mass of
             the leptoquark [Formula presented]. Assuming the decay
             [Formula presented], we exclude scalar leptoquarks for
             [Formula presented], and vector leptoquarks for [Formula
             presented] and coupling which produces the minimum cross
             section, at a [Formula presented] confidence level. © 2002
             The American Physical Society.},
   Doi = {10.1103/PhysRevLett.88.191801},
   Key = {fds308173}
}

@article{fds350338,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA and Pereira,
             RA},
   Title = {Search for light long-lived neutral particles produced in pp
             collisions at √s=13TeV and decaying into collimated
             leptons or light hadrons with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {5},
   Year = {2020},
   Month = {May},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-7997-4},
   Abstract = {Several models of physics beyond the Standard Model predict
             the existence of dark photons, light neutral particles
             decaying into collimated leptons or light hadrons. This
             paper presents a search for long-lived dark photons produced
             from the decay of a Higgs boson or a heavy scalar boson and
             decaying into displaced collimated Standard Model fermions.
             The search uses data corresponding to an integrated
             luminosity of 36.1 fb- 1 collected in proton–proton
             collisions at s=13 Te recorded in 2015–2016 with the
             ATLAS detector at the Large Hadron Collider. The observed
             number of events is consistent with the expected background,
             and limits on the production cross section times branching
             fraction as a function of the proper decay length of the
             dark photon are reported. A cross section times branching
             fraction above 4 pb is excluded for a Higgs boson decaying
             into two dark photons for dark-photon decay lengths between
             1.5 mm and 307 mm.},
   Doi = {10.1140/epjc/s10052-020-7997-4},
   Key = {fds350338}
}

@article{fds356629,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada
             Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O},
   Title = {Search for light resonances decaying to boosted quark pairs
             and produced in association with a photon or a jet in
             proton–proton collisions at √s=13TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {788},
   Pages = {316-335},
   Year = {2019},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.09.062},
   Abstract = {This Letter presents a search for new light resonances
             decaying to pairs of quarks and produced in association with
             a high-pT photon or jet. The dataset consists of
             proton–proton collisions with an integrated luminosity of
             36.1 fb−1 at a centre-of-mass energy of s=13 TeV recorded
             by the ATLAS detector at the Large Hadron Collider.
             Resonance candidates are identified as massive large-radius
             jets with substructure consistent with a particle decaying
             into a quark pair. The mass spectrum of the candidates is
             examined for local excesses above background. No evidence of
             a new resonance is observed in the data, which are used to
             exclude the production of a lepto-phobic axial-vector Z′
             boson.},
   Doi = {10.1016/j.physletb.2018.09.062},
   Key = {fds356629}
}

@article{fds307673,
   Author = {ATLAS Collaboration},
   Title = {Search for light top squark pair production in final states
             with leptons and b-jets with the ATLAS detector in sqrt(s) =
             7 TeV proton-proton collisions},
   Journal = {Physics Letters B},
   Volume = {72},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2012},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2237-1},
   Abstract = {A search is presented for the pair production of light
             scalar top quarks in √s = 7 TeV proton–proton collisions
             recorded with the ATLAS detector at the Large Hadron
             Collider. This analysis uses the full data sample collected
             during 2011 running that corresponds to a total integrated
             luminosity of 4.7 fb−1. Light scalar top quarks are
             searched for in events with two opposite-sign leptons (e,
             μ), large missing transverse momentum and at least one jet
             in the final state. No excess over Standard Model
             expectations is found, and the results are interpreted under
             the assumption that the light scalar top decays to a b-quark
             in addition to an on-shell chargino whose decay occurs
             through a virtual W boson. If the chargino mass is 106 GeV,
             light scalar top-quark masses up to 130 GeV are excluded for
             neutralino masses below 70 GeV.},
   Doi = {10.1140/epjc/s10052-012-2237-1},
   Key = {fds307673}
}

@article{fds307610,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Search for light top squark pair production in final states
             with leptons and b-jets with the ATLAS detector in √s=7
             TeV proton–proton collisions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {720},
   Number = {1-3},
   Pages = {13-31},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.049},
   Abstract = {The results of a search for pair production of light top
             squarks are presented, using 4.7 fb−1 of s=7 TeV
             proton–proton collisions collected with the ATLAS detector
             at the Large Hadron Collider. This search targets top
             squarks with masses similar to, or lighter than, the top
             quark mass. Final states containing exclusively one or two
             leptons (e,μ), large missing transverse momentum,
             light-flavour jets and b-jets are used to reconstruct the
             top squark pair system. Event-based mass scale variables are
             used to separate the signal from a large tt¯ background. No
             excess over the Standard Model expectations is found. The
             results are interpreted in the framework of the Minimal
             Supersymmetric Standard Model, assuming the top squark
             decays exclusively to a chargino and a b-quark, while
             requiring different mass relationships between the
             Supersymmetric particles in the decay chain. Light top
             squarks with masses between 123–167 GeV are excluded for
             neutralino masses around 55 GeV.},
   Doi = {10.1016/j.physletb.2013.01.049},
   Key = {fds307610}
}

@article{fds356681,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
             LJ},
   Title = {Search for long-lived charginos based on a
             disappearing-track signature in pp collisions at √s=13 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {6},
   Year = {2018},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2018)022},
   Abstract = {This paper presents a search for direct electroweak gaugino
             or gluino pair production with a chargino nearly
             mass-degenerate with a stable neutralino. It is based on an
             integrated luminosity of 36.1 fb−1 of pp collisions at
             s=13 TeV collected by the ATLAS experiment at the LHC. The
             final state of interest is a disappearing track accompanied
             by at least one jet with high transverse momentum from
             initial-state radiation or by four jets from the gluino
             decay chain. The use of short track segments reconstructed
             from the innermost tracking layers significantly improves
             the sensitivity to short chargino lifetimes. The results are
             found to be consistent with Standard Model predictions.
             Exclusion limits are set at 95% confidence level on the mass
             of charginos and gluinos for different chargino lifetimes.
             For a pure wino with a lifetime of about 0.2 ns, chargino
             masses up to 460 GeV are excluded. For the strong production
             channel, gluino masses up to 1.65 TeV are excluded assuming
             a chargino mass of 460 GeV and lifetime of 0.2 ns.[Figure
             not available: see fulltext.].},
   Doi = {10.1007/JHEP06(2018)022},
   Key = {fds356681}
}

@article{fds364957,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S and Arling, JH},
   Title = {Search for long-lived charginos based on a
             disappearing-track signature using 136 fb - 1 of
             pp collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {82},
   Number = {7},
   Year = {2022},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-022-10489-5},
   Abstract = {A search for long-lived charginos produced either directly
             or in the cascade decay of heavy prompt gluino states is
             presented. The search is based on proton–proton collision
             data collected at a centre-of-mass energy of s = 13 TeV
             between 2015 and 2018 with the ATLAS detector at the LHC,
             corresponding to an integrated luminosity of 136 fb- 1.
             Long-lived charginos are characterised by a distinct
             signature of a short and then disappearing track, and are
             reconstructed using at least four measurements in the ATLAS
             pixel detector, with no subsequent measurements in the
             silicon-microstrip tracking volume nor any associated energy
             deposits in the calorimeter. The final state is complemented
             by a large missing transverse-momentum requirement for
             triggering purposes and at least one high-transverse-momentum
             jet. No excess above the expected backgrounds is observed.
             Exclusion limits are set at 95% confidence level on the
             masses of the chargino and gluino for different chargino
             lifetimes. Chargino masses up to 660 (210) GeV are
             excluded in scenarios where the chargino is a pure wino
             (higgsino). For charginos produced during the cascade decay
             of a heavy gluino, gluinos with masses below 2.1 TeV are
             excluded for a chargino mass of 300 GeV and a lifetime of
             0.2 ns.},
   Doi = {10.1140/epjc/s10052-022-10489-5},
   Key = {fds364957}
}

@article{fds308130,
   Author = {al, AVKWDAE},
   Title = {Search for Long-Lived Doubly-Charged Higgs Bosons in P
             anti-P Collisions at s**(1/2) = 1.96 TeV},
   Journal = {Physical Review Letters},
   Volume = {95},
   Number = {071801},
   Year = {2005},
   Month = {August},
   Key = {fds308130}
}

@article{fds307949,
   Author = {Aaltonen, T and others},
   Title = {Search for Long-Lived Massive Charged Particles in 1.96 TeV
             pp̅ Collisions},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {2},
   Pages = {021802},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.021802},
   Abstract = {We performed a signature-based search for long-lived charged
             massive particles produced in 1.0  fb-1 of pp̅
             collisions at sqrt[s]=1.96  TeV, collected with the CDF
             II detector using a high transverse-momentum (pT) muon
             trigger. The search used time of flight to isolate slowly
             moving, high-pT particles. One event passed our selection
             cuts with an expected background of 1.9 &plusmn; 0.2 events.
             We set an upper bound on the production cross section and,
             interpreting this result within the context of a stable
             scalar top-quark model, set a lower limit on the particle
             mass of 249  GeV/c2 at 95% C.L.},
   Doi = {10.1103/physrevlett.103.021802},
   Key = {fds307949}
}

@article{fds310347,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for long-lived neutral particles decaying into lepton
             jets in proton-proton collisions at √s= 8TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP11(2014)088},
   Abstract = {Abstract: Several models of physics beyond the Standard
             Model predict neutral particles that decay into final states
             consisting of collimated jets of light leptons and hadrons
             (so-called “lepton jets”). These particles can also be
             long-lived with decay length comparable to, or even larger
             than, the LHC detectors’ linear dimensions. This paper
             presents the results of a search for lepton jets in
             proton-proton collisions at the centre-of-mass energy of
             √s= 8TeV in a sample of 20.3 fb−1 collected during 2012
             with the ATLAS detector at the LHC. Limits on models
             predicting Higgs boson decays to neutral long-lived lepton
             jets are derived as a function of the particle’s proper
             decay length.},
   Doi = {10.1007/JHEP11(2014)088},
   Key = {fds310347}
}

@article{fds356592,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger,
             M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou,
             C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Estevez, MA and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
             VA and Pereira, RA and Arce, ATH and Arduh, FA and Arguin,
             JF},
   Title = {Search for long-lived neutral particles in pp collisions at
             √s=13TeV that decay into displaced hadronic jets in the
             ATLAS calorimeter},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {6},
   Year = {2019},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-6962-6},
   Abstract = {This paper describes a search for pairs of neutral,
             long-lived particles decaying in the ATLAS calorimeter.
             Long-lived particles occur in many extensions to the
             Standard Model and may elude searches for new promptly
             decaying particles. The analysis considers neutral,
             long-lived scalars with masses between 5 and 400 GeV,
             produced from decays of heavy bosons with masses between 125
             and 1000 GeV, where the long-lived scalars decay into
             Standard Model fermions. The analysis uses either 10.8fb-1
             or 33.0fb-1 of data (depending on the trigger) recorded in
             2016 at the LHC with the ATLAS detector in proton–proton
             collisions at a centre-of-mass energy of 13 TeV. No
             significant excess is observed, and limits are reported on
             the production cross section times branching ratio as a
             function of the proper decay length of the long-lived
             particles.},
   Doi = {10.1140/epjc/s10052-019-6962-6},
   Key = {fds356592}
}

@article{fds349432,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH},
   Title = {Search for long-lived neutral particles produced in pp
             collisions at s =13 TeV decaying into displaced hadronic
             jets in the ATLAS inner detector and muon
             spectrometer},
   Journal = {Physical Review D},
   Volume = {101},
   Number = {5},
   Year = {2020},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.101.052013},
   Abstract = {A search is presented for pair production of long-lived
             neutral particles using 33 fb-1 of s=13 TeV proton-proton
             collision data, collected during 2016 by the ATLAS detector
             at the LHC. This search focuses on a topology in which one
             long-lived particle decays in the ATLAS inner detector and
             the other decays in the muon spectrometer. Special
             techniques are employed to reconstruct the displaced tracks
             and vertices in the inner detector and in the muon
             spectrometer. One event is observed that passes the full
             event selection, which is consistent with the estimated
             background. Limits are placed on scalar boson propagators
             with masses from 125 GeV to 1000 GeV decaying into pairs of
             long-lived hidden-sector scalars with masses from 8 GeV to
             400 GeV. The limits placed on several low-mass scalars
             extend previous exclusion limits in the range of proper
             lifetimes cτ from 5 cm to 1 m.},
   Doi = {10.1103/PhysRevD.101.052013},
   Key = {fds349432}
}

@article{fds347448,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
   Title = {Search for long-lived particles in final states with
             displaced dimuon vertices in pp collisions at s =13 TeV with
             the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {99},
   Number = {1},
   Year = {2019},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.99.012001},
   Abstract = {A search is performed for a long-lived particle decaying
             into a final state that includes a pair of muons of
             opposite-sign electric charge, using proton-proton collision
             data collected at s=13 TeV by the ATLAS detector at the
             Large Hadron Collider corresponding to an integrated
             luminosity of 32.9 fb-1. No significant excess over the
             Standard Model expectation is observed. Limits at 95%
             confidence level on the lifetime of the long-lived particle
             are presented in models of new phenomena including
             gauge-mediated supersymmetry or decay of the Higgs boson, H,
             to a pair of dark photons, ZD. Lifetimes in the range
             cτ=1-2400 cm are excluded, depending on the parameters of
             the model. In the supersymmetric model, the lightest
             neutralino is the next-to-lightest supersymmetric particle,
             with a relatively long lifetime due to its weak coupling to
             the gravitino, the lightest supersymmetric particle. The
             lifetime limits are determined for very light gravitino mass
             and various assumptions for the neutralino mass in the range
             300-1000 GeV. In the dark photon model, the lifetime limits
             are interpreted as exclusion contours in the plane of the
             coupling between the ZD and the Standard Model Z boson
             versus the ZD mass (in the range 20-60 GeV), for various
             assumptions for the H→ZDZD branching fraction.},
   Doi = {10.1103/PhysRevD.99.012001},
   Key = {fds347448}
}

@article{fds356620,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Search for long-lived particles produced in pp collisions at
             s =13 TeV that decay into displaced hadronic jets in the
             ATLAS muon spectrometer},
   Journal = {Physical Review D},
   Volume = {99},
   Number = {5},
   Year = {2019},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.99.052005},
   Abstract = {A search for the decay of neutral, weakly interacting,
             long-lived particles using data collected by the ATLAS
             detector at the LHC is presented. The analysis in this paper
             uses 36.1 fb-1 of proton-proton collision data at s=13 TeV
             recorded in 2015-2016. The search employs techniques for
             reconstructing vertices of long-lived particles decaying
             into jets in the muon spectrometer exploiting a two-vertex
             strategy and a novel technique that requires only one vertex
             in association with additional activity in the detector that
             improves the sensitivity for longer lifetimes. The observed
             numbers of events are consistent with the expected
             background and limits for several benchmark signals are
             determined.},
   Doi = {10.1103/PhysRevD.99.052005},
   Key = {fds356620}
}

@article{fds311113,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {Search for long-lived stopped R-hadrons decaying out of time
             with pp collisions using the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {11},
   Pages = {112003-1-112003-30},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.112003},
   Abstract = {An updated search is performed for gluino, top squark, or
             bottom squark R-hadrons that have come to rest within the
             ATLAS calorimeter, and decay at some later time to hadronic
             jets and a neutralino, using 5.0 and 22:9 fb-1 of pp
             collisions at 7 and 8 TeV, respectively. Candidate decay
             events are triggered in selected empty bunch crossings of
             the LHC in order to remove pp collision backgrounds.
             Selections based on jet shape and muon system activity are
             applied to discriminate signal events from cosmic ray and
             beam-halo muon backgrounds. In the absence of an excess of
             events, improved limits are set on gluino, stop, and sbottom
             masses for different decays, lifetimes, and neutralino
             masses. With a neutralino of mass 100 GeV, the analysis
             excludes gluinos with mass below 832 GeV (with an expected
             lower limit of 731 GeV), for a gluino lifetime between 10
             μs and 1000 s in the generic R-hadron model with equal
             branching ratios for decays to (formula presented) and
             (formula presented). Under the same assumptions for the
             neutralino mass and squark lifetime, top squarks and bottom
             squarks in the Regge R-hadron model are excluded with masses
             below 379 and 344 GeV, respectively.},
   Doi = {10.1103/PhysRevD.88.112003},
   Key = {fds311113}
}

@article{fds307622,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, JF and Arik, E},
   Title = {Search for long-lived, heavy particles in final states with
             a muon and multi-track displaced vertex in proton-proton
             collisions at √s=7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {719},
   Number = {4-5},
   Pages = {280-298},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.042},
   Abstract = {Many extensions of the Standard Model posit the existence of
             heavy particles with long lifetimes. In this Letter, results
             are presented of a search for events containing one or more
             such particles, which decay at a significant distance from
             their production point, using a final state containing
             charged hadrons and an associated muon. This analysis uses a
             data sample of proton-proton collisions at s=7TeV
             corresponding to an integrated luminosity of 4.4 fb−1
             collected in 2011 by the ATLAS detector operating at the
             Large Hadron Collider. Results are interpreted in the
             context of R-parity violating supersymmetric scenarios. No
             events in the signal region are observed and limits are set
             on the production cross section for pair production of
             supersymmetric particles, multiplied by the square of the
             branching fraction for a neutralino to decay to charged
             hadrons and a muon, based on the scenario where both of the
             produced supersymmetric particles give rise to neutralinos
             that decay in this way. However, since the search strategy
             is based on triggering on and reconstructing the decay
             products of individual long-lived particles, irrespective of
             the rest of the event, these limits can easily be
             reinterpreted in scenarios with different numbers of
             long-lived particles per event. The limits are presented as
             a function of neutralino lifetime, and for a range of squark
             and neutralino masses.},
   Doi = {10.1016/j.physletb.2013.01.042},
   Key = {fds307622}
}

@article{fds353484,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
             Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V},
   Title = {Search for long-lived, massive particles in events with a
             displaced vertex and a muon with large impact parameter in
             pp collisions at s =13 TeV with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {102},
   Number = {3},
   Year = {2020},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.102.032006},
   Abstract = {A search for long-lived particles decaying into hadrons and
             at least one muon is presented. The analysis selects events
             that pass a muon or missing-transverse-momentum trigger and
             contain a displaced muon track and a displaced vertex. The
             analyzed dataset of proton-proton collisions at s=13 TeV was
             collected with the ATLAS detector and corresponds to 136
             fb-1. The search employs dedicated reconstruction techniques
             that significantly increase the sensitivity to long-lived
             particle decays that occur in the ATLAS inner detector.
             Background estimates for Standard Model processes and
             instrumental effects are extracted from data. The observed
             event yields are compatible with those expected from
             background processes. The results are presented as limits at
             95% confidence level on model-independent cross sections for
             processes beyond the Standard Model, and interpreted as
             exclusion limits in scenarios with pair production of
             long-lived top squarks that decay via a small
             R-parity-violating coupling into a quark and a muon. Top
             squarks with masses up to 1.7 TeV are excluded for a
             lifetime of 0.1 ns, and masses below 1.3 TeV are excluded
             for lifetimes between 0.01 ns and 30 ns.},
   Doi = {10.1103/PhysRevD.102.032006},
   Key = {fds353484}
}

@article{fds356694,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
             LJ},
   Title = {Search for long-lived, massive particles in events with
             displaced vertices and missing transverse momentum in √s =
             13 TeV pp collisions with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {97},
   Number = {5},
   Year = {2018},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.97.052012},
   Abstract = {A search for long-lived, massive particles predicted by many
             theories beyond the Standard Model is presented. The search
             targets final states with large missing transverse momentum
             and at least one high-mass displaced vertex with five or
             more tracks, and uses 32.8 fb-1 of s=13 TeV pp collision
             data collected by the ATLAS detector at the LHC. The
             observed yield is consistent with the expected background.
             The results are used to extract 95% C.L. exclusion limits on
             the production of long-lived gluinos with masses up to 2.37
             TeV and lifetimes of O(10-2)-O(10) ns in a simplified model
             inspired by split supersymmetry.},
   Doi = {10.1103/PhysRevD.97.052012},
   Key = {fds356694}
}

@article{fds356788,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
             ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
             S and Arik, E and Arik, M},
   Title = {Search for long-lived, multi-charged particles in pp
             collisions at √s=7 TeV using the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {722},
   Number = {4-5},
   Pages = {305-323},
   Year = {2013},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.04.036},
   Abstract = {A search for highly ionising, penetrating particles with
             electric charges from |q|=2e to 6e is performed using the
             ATLAS detector at the CERN Large Hadron Collider.
             Proton-proton collision data taken at s=7 TeV during the
             2011 running period, corresponding to an integrated
             luminosity of 4.4 fb−1, are analysed. No signal candidates
             are observed, and 95% confidence level cross-section upper
             limits are interpreted as mass-exclusion lower limits for a
             simplified Drell–Yan production model. In this model,
             masses are excluded from 50 GeV up to 430, 480, 490, 470 and
             420 GeV for charges 2e, 3e, 4e, 5e and 6e,
             respectively.},
   Doi = {10.1016/j.physletb.2013.04.036},
   Key = {fds356788}
}

@article{fds310275,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for long-lived, weakly interacting particles that
             decay to displaced hadronic jets in proton-proton collisions
             at s =8 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.012010},
   Abstract = {A search for the decay of neutral, weakly interacting,
             long-lived particles using data collected by the ATLAS
             detector at the LHC is presented. This analysis uses the
             full data set recorded in 2012: 20.3 fb-1 of proton-proton
             collision data at s=8 TeV. The search employs techniques for
             reconstructing decay vertices of long-lived particles
             decaying to jets in the inner tracking detector and muon
             spectrometer. Signal events require at least two
             reconstructed vertices. No significant excess of events over
             the expected background is found, and limits as a function
             of proper lifetime are reported for the decay of the Higgs
             boson and other scalar bosons to long-lived particles and
             for Hidden Valley Z′ and Stealth SUSY benchmark models.
             The first search results for displaced decays in Z′ and
             Stealth SUSY models are presented. The upper bounds of the
             excluded proper lifetimes are the most stringent to
             date.},
   Doi = {10.1103/PhysRevD.92.012010},
   Key = {fds310275}
}

@article{fds347458,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik,
             Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
             M and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
             A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary,
             O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund,
             O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RMB and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
             TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
             KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt,
             A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
             DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
             D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
             BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
             S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M},
   Title = {Search for Low-Mass Dijet Resonances Using Trigger-Level
             Jets with the ATLAS Detector in pp Collisions at
             sqrt[s]=13  TeV.},
   Journal = {Physical review letters},
   Volume = {121},
   Number = {8},
   Pages = {081801},
   Year = {2018},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.121.081801},
   Abstract = {Searches for dijet resonances with sub-TeV masses using the
             ATLAS detector at the Large Hadron Collider can be
             statistically limited by the bandwidth available to
             inclusive single-jet triggers, whose data-collection rates
             at low transverse momentum are much lower than the rate from
             standard model multijet production. This Letter describes a
             new search for dijet resonances where this limitation is
             overcome by recording only the event information calculated
             by the jet trigger algorithms, thereby allowing much higher
             event rates with reduced storage needs. The search targets
             low-mass dijet resonances in the range 450-1800 GeV. The
             analyzed data set has an integrated luminosity of up to
             29.3  fb^{-1} and was recorded at a center-of-mass
             energy of 13 TeV. No excesses are found; limits are set on
             Gaussian-shaped contributions to the dijet mass distribution
             from new particles and on a model of dark-matter particles
             with axial-vector couplings to quarks.},
   Doi = {10.1103/physrevlett.121.081801},
   Key = {fds347458}
}

@article{fds347551,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
             Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
             NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
             AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini,
             MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras,
             D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V},
   Title = {Search for low-mass resonances decaying into two jets and
             produced in association with a photon using pp collisions at
             s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {795},
   Pages = {56-75},
   Year = {2019},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.03.067},
   Abstract = {A search is performed for localised excesses in dijet mass
             distributions of low-dijet-mass events produced in
             association with a high transverse energy photon. The search
             uses up to 79.8 fb−1 of LHC proton–proton collisions
             collected by the ATLAS experiment at a centre-of-mass energy
             of 13 TeV during 2015–2017. Two variants are presented:
             one which makes no jet flavour requirements and one which
             requires both jets to be tagged as b-jets. The observed mass
             distributions are consistent with multi-jet processes in the
             Standard Model. The data are used to set upper limits on the
             production cross-section for a benchmark Z′ model and,
             separately, on generic Gaussian-shape contributions to the
             mass distributions, extending the current ATLAS constraints
             on dijet resonances to the mass range between 225 and 1100
             GeV.},
   Doi = {10.1016/j.physletb.2019.03.067},
   Key = {fds347551}
}

@article{fds310276,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
             G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for low-scale gravity signatures in multi-jet final
             states with the ATLAS detector at √s =
             8TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {7},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2015)032},
   Abstract = {A search for evidence of physics beyond the Standard Model
             in final states with multiple high-transverse-momentum jets
             is performed using 20.3 fb−1 of proton-proton collision
             data at (Formula presented.) = 8 TeV recorded by the ATLAS
             detector at the LHC. No significant excess of events beyond
             Standard Model expectations is observed, and upper limits on
             the visible cross sections for non-Standard Model production
             of multi-jet final states are set. A wide variety of models
             for black hole and string ball production and decay are
             considered, and the upper limit on the cross section times
             acceptance is as low as 0.16 fb at the 95% confidence level.
             For these models, excluded regions are also given as
             function of the main model parameters.},
   Doi = {10.1007/JHEP07(2015)032},
   Key = {fds310276}
}

@article{fds348981,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
             Pereira, R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin,
             J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O and Arnold, H and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
             M and Atlay, NB and Atmani, H and Augsten, K and Avolio, G and Avramidou,
             R and Ayoub, MK and Azoulay, AM and Azuelos, G and Baca, MJ and Bachacou,
             H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bajic,
             M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura,
             AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barsov, S and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Berry, T and Berta, P and Bertella, C and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
             M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bitadze, A and Bittrich, C and Bjørke, K and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
             V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borecka-Bielska, HM and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
             WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock,
             I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burr, JTP and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, FC and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carter, JWS and Casado, MP and Casha, AF and Casper,
             DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro,
             NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chakraborty, D and Chan, SK and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen,
             Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias,
             TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ},
   Title = {Search for Magnetic Monopoles and Stable
             High-Electric-Charge Objects in 13 Tev Proton-Proton
             Collisions with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {124},
   Number = {3},
   Pages = {031802},
   Year = {2020},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.124.031802},
   Abstract = {A search for magnetic monopoles and high-electric-charge
             objects is presented using 34.4  fb^{-1} of 13 TeV pp
             collision data collected by the ATLAS detector at the LHC
             during 2015 and 2016. The considered signature is based upon
             high ionization in the transition radiation tracker of the
             inner detector associated with a pencil-shape energy deposit
             in the electromagnetic calorimeter. The data were collected
             by a dedicated trigger based on the tracker high-threshold
             hit capability. The results are interpreted in models of
             Drell-Yan pair production of stable particles with two spin
             hypotheses (0 and 1/2) and masses ranging from 200 to
             4000 GeV. The search improves by approximately a factor of
             5 the constraints on the direct production of magnetic
             monopoles carrying one or two Dirac magnetic charges and
             stable objects with electric charge in the range
             20≤|z|≤60 and extends the charge range to
             60<|z|≤100.},
   Doi = {10.1103/physrevlett.124.031802},
   Key = {fds348981}
}

@article{fds315362,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for magnetic monopoles and stable particles with high
             electric charges in 8 TeV pp collisions with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {March},
   ISSN = {2470-0010},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.052009},
   Abstract = {A search for highly ionizing particles produced in
             proton-proton collisions at 8 TeV center-of-mass energy is
             performed by the ATLAS Collaboration at the CERN Large
             Hadron Collider. The data set used corresponds to an
             integrated luminosity of 7.0 fb-1. A customized trigger
             significantly increases the sensitivity, permitting a search
             for such particles with charges and energies beyond what was
             previously accessible. No events were found in the signal
             region, leading to production cross section upper limits in
             the mass range 200-2500 GeV for magnetic monopoles with
             magnetic charge in the range 0.5gD<|g|<2.0gD, where gD is
             the Dirac charge, and for stable particles with electric
             charge in the range 10<|z|<60. Model-dependent limits are
             presented in given pair-production scenarios, and
             model-independent limits are presented in fiducial regions
             of particle energy and pseudorapidity.},
   Doi = {10.1103/PhysRevD.93.052009},
   Key = {fds315362}
}

@article{fds307654,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert,
             B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou,
             R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Begel, M and Behar Harpaz and S and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
             A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J},
   Title = {Search for magnetic monopoles in sqrt[s]=7  TeV pp
             collisions with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {26},
   Pages = {261803},
   Year = {2012},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.109.261803},
   Abstract = {This Letter presents a search for magnetic monopoles with
             the ATLAS detector at the CERN Large Hadron Collider using
             an integrated luminosity of 2.0  fb(-1) of pp collisions
             recorded at a center-of-mass energy of sqrt[s]=7  TeV.
             No event is found in the signal region, leading to an upper
             limit on the production cross section at 95% confidence
             level of 1.6/ϵ  fb for Dirac magnetic monopoles with
             the minimum unit magnetic charge and with mass between 200
             GeV and 1500 GeV, where ϵ is the monopole reconstruction
             efficiency. The efficiency ϵ is high and uniform in the
             fiducial region given by pseudorapidity |η|<1.37 and
             transverse kinetic energy 600-700<E(kin)sinθ<1400  GeV.
             The minimum value of 700 GeV is for monopoles of mass 200
             GeV, whereas the minimum value of 600 GeV is applicable for
             higher mass monopoles. Therefore, the upper limit on the
             production cross section at 95% confidence level is 2 fb in
             this fiducial region. Assuming the kinematic distributions
             from Drell-Yan pair production of spin-1/2 Dirac magnetic
             monopoles, the efficiency is in the range 1%-10%, leading to
             an upper limit on the cross section at 95% confidence level
             that varies from 145 fb to 16 fb for monopoles with mass
             between 200 GeV and 1200 GeV. This limit is weaker than the
             fiducial limit because most of these monopoles lie outside
             the fiducial region.},
   Doi = {10.1103/physrevlett.109.261803},
   Key = {fds307654}
}

@article{fds372888,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
             J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury,
             KA and Alberghi, GL and Albert, J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
             Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
             C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
             M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
             SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
   Title = {Search for Majorana neutrinos in same-sign WW scattering
             events from pp collisions at √s=13 TeV},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {9},
   Year = {2023},
   Month = {September},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11915-y},
   Abstract = {A search for Majorana neutrinos in same-sign WW scattering
             events is presented. The analysis uses s=13 TeV
             proton–proton collision data with an integrated luminosity
             of 140 fb - 1 recorded during 2015–2018 by the ATLAS
             detector at the Large Hadron Collider. The analysis targets
             final states including exactly two same-sign muons and at
             least two hadronic jets well separated in rapidity. The
             modelling of the main backgrounds, from Standard Model
             same-sign WW scattering and WZ production, is constrained
             with data in dedicated signal-depleted control regions. The
             distribution of the transverse momentum of the
             second-hardest muon is used to search for signals
             originating from a heavy Majorana neutrino with a mass
             between 50 GeV and 20 TeV. No significant excess is
             observed over the background expectation. The results are
             interpreted in a benchmark scenario of the Phenomenological
             Type-I Seesaw model. In addition, the sensitivity to the
             Weinberg operator is investigated. Upper limits at the 95%
             confidence level are placed on the squared
             muon-neutrino–heavy-neutrino mass-mixing matrix element |
             VμN| 2 as a function of the heavy Majorana neutrino’s
             mass mN , and on the effective μμ Majorana neutrino mass |
             mμμ| .},
   Doi = {10.1140/epjc/s10052-023-11915-y},
   Key = {fds372888}
}

@article{fds325310,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TP and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amoros, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
             G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimaraes da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
             N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Boeser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler,
             S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans,
             G and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Buescher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth,
             JM and Buttinger, W and Urban, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido,
             MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro,
             NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan,
             M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall,
             J},
   Title = {Search for massive colored scalars in four-jet final states
             in √s=7 TeV proton-proton collisions with the ATLAS
             detector},
   Journal = {EUROPEAN PHYSICAL JOURNAL C},
   Volume = {71},
   Number = {12},
   Publisher = {Springer New York LLC},
   Year = {2011},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1828-6},
   Abstract = {A search for pair-produced scalar particles decaying to a
             four-jet final state is presented. The analysis is performed
             using an integrated luminosity of 34 pb-1 recorded by the
             ATLAS detector in 2010. No deviation from the Standard Model
             is observed. For a scalar mass of 100 GeV (190 GeV) the
             limit on the scalar gluon pair production cross section at
             95% confidence level is 1 nb (0.28 nb). When these results
             are interpreted as mass limits, scalar-gluons (hyperpions)
             with masses of 100 to 185 GeV (100 to 155 GeV) are excluded
             at 95% confidence level with the exception of a mass window
             of width about 5 GeV (15 GeV) around 140
             GeV.},
   Doi = {10.1140/epjc/s10052-011-1828-6},
   Key = {fds325310}
}

@article{fds310280,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for massive supersymmetric particles decaying to many
             jets using the ATLAS detector in pp collisions at s =8
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.112016},
   Abstract = {Results of a search for decays of massive particles to fully
             hadronic final states are presented. This search uses 20.3
             fb-1 of data collected by the ATLAS detector in s=8 TeV
             proton-proton collisions at the LHC. Signatures based on
             high jet multiplicities without requirements on the missing
             transverse momentum are used to search for
             R-parity-violating supersymmetric gluino pair production
             with subsequent decays to quarks. The analysis is performed
             using a requirement on the number of jets, in combination
             with separate requirements on the number of b-tagged jets,
             as well as a topological observable formed from the scalar
             sum of the mass values of large-radius jets in the event.
             Results are interpreted in the context of all possible
             branching ratios of direct gluino decays to various quark
             flavors. No significant deviation is observed from the
             expected Standard Model backgrounds estimated using jet
             counting as well as data-driven templates of the
             total-jet-mass spectra. Gluino pair decays to ten or more
             quarks via intermediate neutralinos are excluded for a
             gluino with mass mg<1 TeV for a neutralino mass mχ10=500
             GeV. Direct gluino decays to six quarks are excluded for
             mg<917 GeV for light-flavor final states, and results for
             various flavor hypotheses are presented.},
   Doi = {10.1103/PhysRevD.91.112016},
   Key = {fds310280}
}

@article{fds313606,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for massive, long-lived particles using multitrack
             displaced vertices or displaced lepton pairs in pp
             collisions at s =8 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {October},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.072004},
   Abstract = {Many extensions of the Standard Model posit the existence of
             heavy particles with long lifetimes. This article presents
             the results of a search for events containing at least one
             long-lived particle that decays at a significant distance
             from its production point into two leptons or into five or
             more charged particles. This analysis uses a data sample of
             proton-proton collisions at s=8 TeV corresponding to an
             integrated luminosity of 20.3 fb-1 collected in 2012 by the
             ATLAS detector operating at the Large Hadron Collider. No
             events are observed in any of the signal regions, and limits
             are set on model parameters within supersymmetric scenarios
             involving R-parity violation, split supersymmetry, and gauge
             mediation. In some of the search channels, the trigger and
             search strategy are based only on the decay products of
             individual long-lived particles, irrespective of the rest of
             the event. In these cases, the provided limits can easily be
             reinterpreted in different scenarios.},
   Doi = {10.1103/PhysRevD.92.072004},
   Key = {fds313606}
}

@article{fds307961,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
             T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
             F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bar-Shalom, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar, P and Behari, S and Bellettini, G and Bellinger,
             J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry,
             T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
             S and Deisher, A and De Lentdecker and G and De Lorenzo and G and Dell'orso,
             M and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent,
             PF and Di Giovanni and GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
             G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia,
             JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber,
             C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker,
             A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun,
             SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato,
             Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim,
             YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson,
             B and Ko, BR and Koay, SA and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus, J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone,
             S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen,
             D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
             P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli,
             F and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, M and Movilla
             Fernandez, P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rajaraman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard,
             PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber,
             I and Sidoti, A and Sinervo, P and Sisakyan, A},
   Title = {Search for maximal flavor violating scalars in same-charge
             lepton pairs in pp collisions at sqrt[s]=1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {4},
   Pages = {041801},
   Year = {2009},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.102.041801},
   Abstract = {Models of maximal flavor violation (MxFV) in elementary
             particle physics may contain at least one new scalar SU(2)
             doublet field Phi(FV)=(eta(0),eta(+)) that couples the first
             and third generation quarks (q_(1), q_(3)) via a Lagrangian
             term L(FV)=xi(13)Phi(FV)q(1)q(3). These models have a
             distinctive signature of same-charge top-quark pairs and
             evade flavor-changing limits from meson mixing measurements.
             Data corresponding to 2 fb(-1) collected by the Collider
             Dectector at Fermilab II detector in pp[over ] collisions at
             sqrt[s]=1.96 TeV are analyzed for evidence of the MxFV
             signature. For a neutral scalar eta(0) with m_(eta;(0))=200
             GeV/c(2) and coupling xi(13)=1, approximately 11 signal
             events are expected over a background of 2.1+/-1.8 events.
             Three events are observed in the data, consistent with
             background expectations, and limits are set on the coupling
             xi(13) for m(eta(0)=180-300 GeV/c(2).},
   Doi = {10.1103/physrevlett.102.041801},
   Key = {fds307961}
}

@article{fds317297,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
   Title = {Search for metastable heavy charged particles with large
             ionisation energy loss in pp collisions at [Formula:
             see text] TeV using the ATLAS experiment.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {9},
   Pages = {407},
   Year = {2015},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3609-0},
   Abstract = {Many extensions of the Standard Model predict the existence
             of charged heavy long-lived particles, such as
             <i>R</i>-hadrons or charginos. These particles, if produced
             at the Large Hadron Collider, should be moving
             non-relativistically and are therefore identifiable through
             the measurement of an anomalously large specific energy loss
             in the ATLAS pixel detector. Measuring heavy long-lived
             particles through their track parameters in the vicinity of
             the interaction vertex provides sensitivity to metastable
             particles with lifetimes from 0.6 ns to 30 ns. A search
             for such particles with the ATLAS detector at the Large
             Hadron Collider is presented, based on a data sample
             corresponding to an integrated luminosity of [Formula: see
             text] fb[Formula: see text] of <i>pp</i> collisions at
             [Formula: see text] TeV. No significant deviation from the
             Standard Model background expectation is observed, and
             lifetime-dependent upper limits on <i>R</i>-hadrons and
             chargino production are set. Gluino <i>R</i>-hadrons with
             10 ns lifetime and masses up to 1185 GeV are excluded at
             95 [Formula: see text] confidence level, and so are
             charginos with 15 ns lifetime and masses up to
             482 GeV.},
   Doi = {10.1140/epjc/s10052-015-3609-0},
   Key = {fds317297}
}

@article{fds321124,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for metastable heavy charged particles with large
             ionization energy loss in pp collisions at s =13 TeV using
             the ATLAS experiment},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.112015},
   Abstract = {This paper presents a search for massive charged long-lived
             particles produced in pp collisions at s=13 TeV at the LHC
             using the ATLAS experiment. The data set used corresponds to
             an integrated luminosity of 3.2 fb-1. Many extensions of the
             Standard Model predict the existence of massive charged
             long-lived particles, such as R-hadrons. These massive
             particles are expected to be produced with a velocity
             significantly below the speed of light, and therefore to
             have a specific ionization higher than any Standard Model
             particle of unit charge at high momenta. The Pixel subsystem
             of the ATLAS detector is used to measure the ionization
             energy loss of reconstructed charged particles and to search
             for such highly ionizing particles. The search presented
             here has much greater sensitivity than a similar search
             performed using the ATLAS detector in the s=8 TeV data set,
             thanks to the increase in expected signal cross section due
             to the higher center-of-mass energy of collisions, to an
             upgraded detector with a new silicon layer close to the
             interaction point, and to analysis improvements. No
             significant deviation from Standard Model background
             expectations is observed, and lifetime-dependent upper
             limits on R-hadron production cross sections and masses are
             set. Gluino R-hadrons with lifetimes above 0.4 ns and
             decaying to qq plus a 100 GeV neutralino are excluded at the
             95% confidence level, with lower mass limit ranging between
             740 and 1590 GeV. In the case of stable R-hadrons the lower
             mass limit at the 95% confidence level is 1570
             GeV.},
   Doi = {10.1103/PhysRevD.93.112015},
   Key = {fds321124}
}

@article{fds310370,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for microscopic black holes and string balls in final
             states with leptons and jets with the ATLAS detector at √s
             = 8 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP08(2014)103},
   Abstract = {A search for an excess of events with multiple high
             transverse momentum objects including charged leptons and
             jets is presented, using 20.3 fb -1 of proton-proton
             collision data recorded by the ATLAS detector at the Large
             Hadron Collider in 2012 at a centre-of-mass energy of √s =
             8 TeV. No excess of events beyond Standard Model
             expectations is observed. Using extra-dimensional models for
             black hole and string ball production and decay, exclusion
             contours are determined as a function of the mass threshold
             for production and the fundamental gravity scale for two,
             four and six extra dimensions. For six extra dimensions,
             mass thresholds of 4.8-6.2 TeV are excluded at 95 %
             confidence level, depending on the fundamental gravity scale
             and model assumptions. Upper limits on the fiducial
             cross-sections for non-Standard Model production of these
             final states are set. [Figure not available: see fulltext.]
             © 2014 The Author(s).},
   Doi = {10.1007/JHEP08(2014)103},
   Key = {fds310370}
}

@article{fds307572,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {Search for microscopic black holes in a like-sign dimuon
             final state using large track multiplicity with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.072001},
   Abstract = {A search is presented for microscopic black holes in a
             like-sign dimuon final state in proton-proton collisions at
             √s=8 TeV. The data were collected with the ATLAS detector
             at the Large Hadron Collider in 2012 and correspond to an
             integrated luminosity of 20.3 fb-1. Using a high track
             multiplicity requirement, 0.6±0.2 background events from
             Standard Model processes are predicted and none observed.
             This result is interpreted in the context of low-scale
             gravity models and 95% C.L. lower limits on microscopic
             black hole masses are set for different model assumptions.
             © 2013 CERN. Published by the American Physical Society
             under the terms of the Creative Commons Attribution 3.0
             License. Further distribution of this work must maintain
             attribution to the author(s) and the published article's
             title, journal citation, and DOI.},
   Doi = {10.1103/PhysRevD.88.072001},
   Key = {fds307572}
}

@article{fds332352,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
             VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Bolton,
             TA and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
             F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and De,
             K and Jong, SJ and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV and Duensing, S and Duflot,
             L},
   Title = {Search for minimal supergravity in single-electron events
             with jets and large missing transverse energy in [Formula
             Presented] collisions at [Formula Presented]},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {66},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.66.112001},
   Abstract = {We describe a search for evidence of minimal supergravity
             (MSUGRA) in [Formula Presented] of data collected with the
             DØ detector at the Fermilab Tevatron [Formula Presented]
             collider at [Formula Presented] Events with a single
             electron, four or more jets, and large missing transverse
             energy were used in this search. The major backgrounds are
             from [Formula Presented] misidentified multijet, [Formula
             Presented] and [Formula Presented] production. We observe no
             excess above the expected number of background events in our
             data. A new limit in terms of MSUGRA model parameters is
             obtained. © 2002 The American Physical Society.},
   Doi = {10.1103/PhysRevD.66.112001},
   Key = {fds332352}
}

@article{fds321075,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali,
             B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Baarreiro Guimrães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Billoud, TRV and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
             A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M},
   Title = {Search for minimal supersymmetric standard model Higgs
             Bosons H / A and for a [Formula: see text] boson in the
             [Formula: see text] final state produced in pp collisions at
             [Formula: see text] TeV with the ATLAS detector.},
   Journal = {Eur Phys J C Part Fields},
   Volume = {76},
   Number = {11},
   Pages = {585},
   Year = {2016},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4400-6},
   Abstract = {A search for neutral Higgs bosons of the minimal
             supersymmetric standard model (MSSM) and for a heavneutral
             [Formula: see text] boson is performed using a data sample
             corresponding to an integrated luminosity of
             3.2 fb[Formula: see text] from proton-proton collisions at
             [Formula: see text]  [Formula: see text] recorded by the
             ATLAS detector at the LHC. The heavy resonance is assumed to
             decay to a [Formula: see text] pair with at least one
             [Formula: see text] lepton decaying to final states with
             hadrons and a neutrino. The search is performed in the mass
             range of 0.2-1.2  [Formula: see text] for the MSSM neutral
             Higgs bosons and 0.5-2.5  [Formula: see text] for the
             heavy neutral [Formula: see text] boson. The data are in
             good agreement with the background predicted by the Standard
             Model. The results are interpreted in MSSM and [Formula: see
             text] benchmark scenarios. The most stringent constraints on
             the MSSM [Formula: see text]-[Formula: see text] space
             exclude at 95 % confidence level (CL) [Formula: see text]
             for [Formula: see text] [Formula: see text] in the
             [Formula: see text] MSSM scenario. For the Sequential
             Standard Model, a [Formula: see text] mass up to
             1.90  [Formula: see text] is excluded at 95 % CL and
             masses up to 1.82-2.17  [Formula: see text] are excluded
             for a [Formula: see text] of the strong flavour
             model.},
   Doi = {10.1140/epjc/s10052-016-4400-6},
   Key = {fds321075}
}

@article{fds307996,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D},
   Title = {Search for narrow resonances lighter than Υ
             mesons},
   Journal = {European Physical Journal C},
   Volume = {62},
   Number = {2},
   Pages = {319-326},
   Publisher = {Springer Nature},
   Year = {2009},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-009-1057-4},
   Abstract = {We report a search for narrow resonances, produced in p p̄
             collisions at √ s=1.96 TeV, that decay into muon pairs
             with invariant mass between 6.3 and 9.0 GeV/c 2. The data,
             collected with the CDF II detector at the Fermilab Tevatron
             collider, correspond to an integrated luminosity of 630 pb
             -1. We use the dimuon invariant mass distribution to set 90%
             upper credible limits of about 1% to the ratio of the
             production cross section times muonic branching fraction of
             possible narrow resonances to that of the Υ(1S) meson. ©
             2009 Springer-Verlag.},
   Doi = {10.1140/epjc/s10052-009-1057-4},
   Key = {fds307996}
}

@article{fds307670,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Lvarez
             González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
             A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
             T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins,
             S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
             JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
             SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
             D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brown, J and Brucken, E and Budagov, J and Bu, XB and Budd, HS and Buehler,
             M and Buescher, V and Bunichev, V and Burdin, S},
   Title = {Search for neutral Higgs bosons in events with multiple
             bottom quarks at the Tevatron},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.091101},
   Abstract = {The combination of searches performed by the CDF and D0
             collaborations at the Fermilab Tevatron Collider for neutral
             Higgs bosons produced in association with b quarks is
             reported. The data, corresponding to 2.6fb -1 of integrated
             luminosity at CDF and 5.2fb -1 at D0, have been collected in
             final states containing three or more b jets. Upper limits
             are set on the cross section multiplied by the branching
             ratio varying between 44 pb and 0.7 pb in the Higgs boson
             mass range 90 to 300 GeV, assuming production of a narrow
             scalar boson. Significant enhancements to the production of
             Higgs bosons can be found in theories beyond the standard
             model, for example, in supersymmetry. The results are
             interpreted as upper limits in the parameter space of the
             minimal supersymmetric standard model in a benchmark
             scenario favoring this decay mode. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.86.091101},
   Key = {fds307670}
}

@article{fds308105,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, J-F and Arisawa, T and Artikov, A and Ashmanskas, W and Attal,
             A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
             J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
             J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Connolly, A and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cruz, A and Cuevas, J and Culbertson, R and Cyr, D and Daronco, S and D'Auria, S and D'onofrio, M and Dagenhart, D and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and Dell'Orso, M and Demers, S and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann, J and Dituro,
             P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers,
             J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
             M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
             LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia, JE and Garcia Sciveres and M and Garfinkel, AF and Gay, C and Gerberich, H and Gerchtein, E and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski,
             D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
             M and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
             da Costa, J and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heijboer, A and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karagoz-Unel, M and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong,
             DJ and Konigsberg, J and Kordas, K and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreps, M and Kreymer, A and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and Lecompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis,
             JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss,
             TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca, G and Margaroli, F and Marginean, R and Marino,
             C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama,
             T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, P and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and von der Mey, M and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman,
             R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Papikonomou, A and Paramonov,
             AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, K and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and van Remortel, N and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Ryan, D and Saarikko, H and Sabik, S and Safonov,
             A and Sakumoto, WK and Salamanna, G and Salto, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
             AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Sexton-Kennedy, L and Sfiligoi,
             I},
   Title = {Search for neutral Higgs bosons of the minimal
             supersymmetric standard model decaying to tau pairs in pp
             collisions at square root of s = 1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {96},
   Number = {1},
   Pages = {011802},
   Year = {2006},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.96.011802},
   Abstract = {We present a search for neutral supersymmetric Higgs bosons
             decaying to tau pairs produced in pp collisions at square
             root of s = 1.96 TeV. The data, corresponding to 310 pb(-1)
             integrated luminosity, were collected with the Collider
             Detector at Fermilab in run II of the Tevatron. No
             significant excess above the standard model backgrounds is
             observed. We set exclusion limits on the production cross
             section times branching fraction to tau pairs for Higgs
             boson masses in the range from 90 to 250
             GeV/c2.},
   Doi = {10.1103/physrevlett.96.011802},
   Key = {fds308105}
}

@article{fds310346,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Search for neutral Higgs bosons of the minimal
             supersymmetric standard model in pp collisions at vs= 8TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {11},
   Pages = {1-47},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2014)056},
   Abstract = {Abstract: A search for the neutral Higgs bosons predicted by
             the Minimal Supersymmetric Standard Model (MSSM) is
             reported. The analysis is performed on data from
             proton-proton collisions at a centre-of-mass energy of 8 TeV
             collected with the ATLAS detector at the Large Hadron
             Collider. The samples used for this search were collected in
             2012 and correspond to integrated luminosities in the range
             19.5-20.3 fb−1. The MSSM Higgs bosons are searched for in
             the τ τ final state. No significant excess over the
             expected background is observed, and exclusion limits are
             derived for the production cross section times branching
             fraction of a scalar particle as a function of its mass. The
             results are also interpreted in the MSSM parameter space for
             various benchmark scenarios.},
   Doi = {10.1007/JHEP11(2014)056},
   Key = {fds310346}
}

@article{fds307862,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Search for neutral MSSM Higgs bosons decaying to
             τ+τ- pairs in proton-proton
             collisions at s=7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {3},
   Pages = {174-192},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.10.001},
   Abstract = {A search for neutral Higgs bosons decaying to pairs of τ
             leptons with the ATLAS detector at the LHC is presented. The
             analysis is based on proton-proton collisions at a
             center-of-mass energy of 7 TeV, recorded in 2010 and
             corresponding to an integrated luminosity of 36 pb-1. After
             signal selection, 276 events are observed in this data
             sample. The observed number of events is consistent with the
             total expected background of 269±36 events. Exclusion
             limits at the 95% confidence level are derived for the
             production cross section of a generic Higgs boson φ as a
             function of the Higgs boson mass and for A/H/h production in
             the Minimal Supersymmetric Standard Model (MSSM) as a
             function of the parameters mA and tanβ. © 2011
             CERN.},
   Doi = {10.1016/j.physletb.2011.10.001},
   Key = {fds307862}
}

@article{fds307834,
   Author = {Aaltonen, TEA},
   Title = {Search for New ${T}^\prime$ Particles in Final States with
             Large Jet Multiplicities and Missing Transverse Energy in
             $p\overline{p}$ Collisions at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {19},
   Pages = {191803},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.191803},
   Abstract = {We present a search for a new particle T' decaying to a top
             quark via T' → t + X, where X goes undetected. We use a
             data sample corresponding to 5.7 fb(-1) of integrated
             luminosity of p p collisions with sqrt[s] = 1.96 TeV,
             collected at Fermilab Tevatron by the CDF II detector. Our
             search for pair production of T' is focused on the hadronic
             decay channel, pp → T'T' → tt + XX → bqq b qq + XX. We
             interpret our results in terms of a model where T' is an
             exotic fourth generation quark and X is a dark matter
             particle. The data are consistent with standard model
             expectations. We set a limit on the generic production of
             T'T' → tt + XX, excluding the fourth generation exotic
             quarks T' at 95% confidence level up to m(T') = 400 GeV/c(2)
             for m(X) ≤ 70 GeV/c(2).},
   Doi = {10.1103/PhysRevLett.107.191803},
   Key = {fds307834}
}

@article{fds307910,
   Author = {Aaltonen, and T, and others},
   Title = {Search for New Bottomlike Quark Pair Decays $Q\bar{Q} \to
             (tW^\mp)(\bar{t}W^\pm)$ in Same-Charge Dilepton
             Events},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {9},
   Pages = {091801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.091801},
   Abstract = {http://arxiv.org/abs/0912.1057},
   Doi = {10.1103/PhysRevLett.104.091801},
   Key = {fds307910}
}

@article{fds307929,
   Author = {Aaltonen, and T, and others},
   Title = {Search for New Color-Octet Vector Particle Decaying to $t
             \bar{t}$ in $p \bar{p}$ Collisions at $\sqrt{s}=1.96$
             TeV},
   Journal = {Phys. Lett.},
   Volume = {B691},
   Number = {4},
   Pages = {183-190},
   Publisher = {Elsevier BV},
   Year = {2010},
   url = {http://dx.doi.org/10.1016/j.physletb.2010.06.036},
   Abstract = {http://arxiv.org/abs/0911.3112},
   Doi = {10.1016/j.physletb.2010.06.036},
   Key = {fds307929}
}

@article{fds307840,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for New Dielectron Resonances and {Randall-Sundrum}
             Gravitons at the {Collider Detector at Fermilab}},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {5},
   Pages = {051801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.051801},
   Abstract = {A search for new dielectron-mass resonances using data
             recorded by the CDF II detector and corresponding to an
             integrated luminosity of 5.7  fb(-1) is presented. No
             significant excess over the expected standard model
             prediction is observed. In this data set, an event with the
             highest dielectron mass ever observed (960  GeV/c(2))
             was recorded. The results are interpreted in the
             Randall-Sundrum (RS) model. Combined with the
             5.4  fb(-1) diphoton analysis, the RS-graviton
             lower-mass limit for the coupling k/M¯(Pl)=0.1 is
             1058  GeV/c(2), making it the strongest limit to
             date.},
   Doi = {10.1103/PhysRevLett.107.051801},
   Key = {fds307840}
}

@article{fds307884,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for new heavy particles decaying to ${ZZ}\rightarrow
             llll$, $lljj$ in $p\overline{p}$ collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {11},
   Pages = {112008},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.112008},
   Abstract = {We report on a search for anomalous production of Z boson
             pairs through a massive resonance decay in data
             corresponding to 2.5-2.9fb-1 of integrated luminosity in
             pp̄ collisions at √s=1.96TeV using the CDF II detector at
             the Fermilab Tevatron. This analysis, with more data and
             channels where the Z bosons decay to muons or jets,
             supersedes the 1.1fb-1 four-electron channel result
             previously published by CDF. In order to maintain high
             efficiency for muons, we use a new forward tracking
             algorithm and muon identification requirements optimized for
             these high signal-to-background channels. Predicting the
             dominant backgrounds in each channel entirely from sideband
             data samples, we observe four-body invariant mass spectra
             above 300GeV/c2 that are consistent with background. We set
             limits using the acceptance for a massive graviton resonance
             that are 7-20 times stronger than the previously published
             direct limits on resonant ZZ diboson production. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.83.112008},
   Key = {fds307884}
}

@article{fds351559,
   Author = {Abulencia, and A, and others},
   Title = {Search for new high mass particles decaying to lepton pairs
             in p anti-p collisions at s**(1/2) = 1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {95},
   Number = {25},
   Pages = {252001},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/physrevlett.95.252001},
   Abstract = {A search for new particles (X) that decay to electron or
             muon pairs has been performed using approximately 200 pb-1
             of pp-bar collision data at sqrt[s]=1.96 TeV collected by
             the CDF II experiment at the Fermilab Tevatron. Limits on
             sigma (pp-bar-->X)BR(X-->ll) are presented as a function of
             dilepton invariant mass mll>150 GeV/c2, for different spin
             hypotheses (0, 1, or 2). The limits are approximately 25 fb
             for mll>600 GeV/c2. Lower mass bounds for X from
             representative models beyond the standard model including
             heavy neutral gauge bosons are presented.},
   Doi = {10.1103/physrevlett.95.252001},
   Key = {fds351559}
}

@article{fds356734,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Search for new high-mass phenomena in the dilepton final
             state using 36 fb−1 of proton-proton collision
             data at √s=13 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {10},
   Year = {2017},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2017)182},
   Abstract = {A search is conducted for new resonant and non-resonant
             high-mass phenomena in dielectron and dimuon final states.
             The search uses 36.1 fb−1 of proton-proton collision data,
             collected at s=13 TeV by the ATLAS experiment at the LHC in
             2015 and 2016. No significant deviation from the Standard
             Model prediction is observed. Upper limits at 95%
             credibility level are set on the cross-section times
             branching ratio for resonances decaying into dileptons,
             which are converted to lower limits on the resonance mass,
             up to 4.1 TeV for the E6-motivated Zχ′. Lower limits on
             the qqℓℓ contact interaction scale are set between 2.4
             TeV and 40 TeV, depending on the model.},
   Doi = {10.1007/JHEP10(2017)182},
   Key = {fds356734}
}

@article{fds353083,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C},
   Title = {Search for new non-resonant phenomena in high-mass dilepton
             final states with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {11},
   Year = {2020},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2020)005},
   Abstract = {A search for new physics with non-resonant signals in
             dielectron and dimuon final states in the mass range above 2
             TeV is presented. This is the first search for non-resonant
             signals in dilepton final states at the LHC to use a
             background estimate from the data. The data, corresponding
             to an integrated luminosity of 139 fb−1, were recorded by
             the ATLAS experiment in proton-proton collisions at a
             center-of-mass energy of s = 13 TeV during Run 2 of the
             Large Hadron Collider. The benchmark signal signature is a
             two-quark and two-lepton contact interaction, which would
             enhance the dilepton event rate at the TeV mass scale. To
             model the contribution from background processes a
             functional form is fit to the dilepton invariant-mass
             spectra in data in a mass region below the region of
             interest. It is then extrapolated to a high-mass signal
             region to obtain the expected background there. No
             significant deviation from the expected background is
             observed in the data. Upper limits at 95% CL on the number
             of events and the visible cross-section times branching
             fraction for processes involving new physics are provided.
             Observed (expected) 95% CL lower limits on the contact
             interaction energy scale reach 35.8 (37.6) TeV. [Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP11(2020)005},
   Key = {fds353083}
}

@article{fds307981,
   Author = {Aaltonen, T and others},
   Title = {Search for new particles decaying into dijets in
             proton-antiproton collisions at sqrt(s) = 1.96
             TeV},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {11},
   Pages = {112002},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.112002},
   Abstract = {We present a search for new particles which produce narrow
             two-jet (dijet) resonances using proton-antiproton collision
             data corresponding to an integrated luminosity of 1.13fb-1
             collected with the CDFA II detector. The measured dijet mass
             spectrum is found to be consistent with next-to-leading-order
             perturbative QCD predictions, and no significant evidence of
             new particles is found. We set upper limits at the 95%
             confidence level on cross sections times the branching
             fraction for the production of new particles decaying into
             dijets with both jets having a rapidity magnitude |y| <1.
             These limits are used to determine the mass exclusions for
             the excited quark, axigluon, flavor-universal coloron, E6
             diquark, color-octet techni-ρ, W′, and Z′. © 2009 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.79.112002},
   Key = {fds307981}
}

@article{fds307726,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli,
             EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
             N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
             R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana,
             S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
             J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani,
             G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Search for new particles decaying to ZZ using final states
             with leptons and jets with the ATLAS detector in √s=7 TeV
             proton-proton collisions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {712},
   Number = {4-5},
   Pages = {331-350},
   Publisher = {Elsevier BV},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.05.020},
   Abstract = {A search is presented for a narrow resonance decaying to a
             pair of Z bosons using data corresponding to 1.02fb-1 of
             integrated luminosity collected by the ATLAS experiment from
             pp collisions at √s=7TeV. Events containing either four
             charged leptons (ℓℓℓℓ) or two charged leptons and
             two jets (ℓℓjj) are analyzed and found to be consistent
             with the Standard Model background expectation. Lower limits
             on a resonance mass are set using the Randall-Sundrum (RS1)
             graviton model as a benchmark. Using both ℓℓℓℓ and
             ℓℓjj events, an RS1 graviton with k/m-pl=0.1 and mass
             between 325 and 845 GeV is excluded at 95% confidence level.
             In addition, the ℓℓℓℓ events are used to set a
             model-independent fiducial cross section limit of
             σfid(pp→X→ZZ)&lt;0.92pb at 95% confidence level for any
             new sources of ZZ production with mZZ greater than 300 GeV.
             © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.05.020},
   Key = {fds307726}
}

@article{fds317302,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for new particles in events with one lepton and
             missing transverse momentum in pp collisions at √s = 8 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {9},
   Pages = {1-42},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2014)037},
   Abstract = {This paper presents a search for new particles in events
             with one lepton (electron or muon) and missing transverse
             momentum using 20.3 fb−1 of proton-proton collision data
             at √s = 8 TeV recorded by the ATLAS experiment at the
             Large Hadron Collider. No significant excess beyond Standard
             Model expectations is observed. A W ′ with Sequential
             Standard Model couplings is excluded at the 95% confidence
             level for masses up to 3.24 TeV. Excited chiral bosons (W*)
             with equivalent coupling strengths are excluded for masses
             up to 3.21 TeV. In the framework of an effective field
             theory limits are also set on the dark matter-nucleon
             scattering cross-section as well as the mass scale M* of the
             unknown mediating interaction for dark matter pair
             production in association with a leptonically decaying
             W.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP09(2014)037},
   Key = {fds317302}
}

@article{fds308067,
   Author = {Aaltonen, and T, and others},
   Title = {Search for New Particles Leading to $Z +$ jets Final States
             in $p \bar{p}$ Collisions at $\sqrt{s}$ =
             1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D76},
   Number = {7},
   Pages = {072006},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.76.072006},
   Abstract = {We present the results of a search for new particles that
             lead to a Z boson plus jets in p[overline p] collisions at
             sqrt(s)=1.96 TeV using the Collider Detector at Fermilab
             (CDF II). A data sample with a luminosity of 1.06 fb-1
             collected using Z boson decays to ee and µµ is used. We
             describe a completely data-based method to predict the
             dominant background from standard model Z+jet events. This
             method can be similarly applied to other analyses requiring
             background predictions in multijet environments, as shown
             when validating the method by predicting the background from
             W+jets in t[overline t] production. No significant excess
             above the background prediction is observed, and a limit is
             set using a fourth generation quark model to quantify the
             acceptance. Assuming BR(b[prime]-->bZ)=100\% and using a
             leading-order calculation of the b[prime] cross section,
             b[prime] quark masses below 268 GeV/c2 are excluded at 95%
             confidence level.},
   Doi = {10.1103/PhysRevD.76.072006},
   Key = {fds308067}
}

@article{fds356737,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for new phenomena in a lepton plus high jet
             multiplicity final state with the ATLAS experiment using
             √s=13 TeV proton-proton collision data},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {9},
   Year = {2017},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2017)088},
   Abstract = {A search for new phenomena in final states characterized by
             high jet multiplicity, an isolated lepton (electron or muon)
             and either zero or at least three b-tagged jets is
             presented. The search uses 36.1 fb−1 of s=13 TeV
             proton-proton collision data collected by the ATLAS
             experiment at the Large Hadron Collider in 2015 and 2016.
             The dominant sources of background are estimated using
             parameterized extrapolations, based on observables at medium
             jet multiplicity, to predict the b-tagged jet multiplicity
             distribution at the higher jet multiplicities used in the
             search. No significant excess over the Standard Model
             expectation is observed and 95% confidence-level limits are
             extracted constraining four simplified models of
             R-parity-violating supersymmetry that feature either gluino
             or top-squark pair production. The exclusion limits reach as
             high as 2.1 TeV in gluino mass and 1.2 TeV in top-squark
             mass in the models considered. In addition, an upper limit
             is set on the cross-section for Standard Model tt¯ tt¯
             production of 60 fb (6.5 × the Standard Model prediction)
             at 95% confidence level. Finally, model-independent limits
             are set on the contribution from new phenomena to the
             signal-region yields.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP09(2017)088},
   Key = {fds356737}
}

@article{fds325794,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali,
             B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
             YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
             S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier,
             S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
             Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M},
   Title = {Search for new phenomena in different-flavour high-mass
             dilepton final states in pp collisions at [Formula:
             see text] Tev with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {10},
   Pages = {541},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4385-1},
   Abstract = {A search is performed for a heavy particle decaying into
             different flavour dilepton pairs ([Formula: see text],
             [Formula: see text] or [Formula: see text]), using
             3.2 fb[Formula: see text] of proton-proton collision data
             at [Formula: see text] TeV collected in 2015 by the ATLAS
             detector at the Large Hadron Collider. No excess over the
             Standard Model prediction is observed. Limits at the 95 %
             credibility level are set on the mass of a [Formula: see
             text] boson with lepton-flavour-violating couplings at 3.0,
             2.7 and 2.6 TeV, and on the mass of a supersymmetric
             [Formula: see text] sneutrino with <i>R</i>-parity-violating
             couplings at 2.3, 2.2 and 1.9 TeV, for [Formula: see text],
             [Formula: see text] and [Formula: see text] final states,
             respectively. The results are also interpreted as limits on
             the threshold mass for quantum black hole
             production.},
   Doi = {10.1140/epjc/s10052-016-4385-1},
   Key = {fds325794}
}

@article{fds310278,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA},
   Title = {Search for New Phenomena in Dijet Angular Distributions in
             Proton-Proton Collisions at sqrt[s]=8 TeV Measured with the
             ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {22},
   Pages = {221802},
   Year = {2015},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.114.221802},
   Abstract = {A search for new phenomena in LHC proton-proton collisions
             at a center-of-mass energy of sqrt[s]=8 TeV was performed
             with the ATLAS detector using an integrated luminosity of
             17.3 fb^{-1}. The angular distributions are studied in
             events with at least two jets; the highest dijet mass
             observed is 5.5 TeV. All angular distributions are
             consistent with the predictions of the standard model. In a
             benchmark model of quark contact interactions, a
             compositeness scale below 8.1 TeV in a destructive
             interference scenario and 12.0 TeV in a constructive
             interference scenario is excluded at 95% C.L.; median
             expected limits are 8.9 TeV for the destructive interference
             scenario and 14.1 TeV for the constructive interference
             scenario.},
   Doi = {10.1103/physrevlett.114.221802},
   Key = {fds310278}
}

@article{fds356740,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Search for new phenomena in dijet events using 37 fb-1 of pp
             collision data collected at √s=13 TeV with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {96},
   Number = {5},
   Year = {2017},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.96.052004},
   Abstract = {Dijet events are studied in the proton-proton collision data
             set recorded at s=13 TeV with the ATLAS detector at the
             Large Hadron Collider in 2015 and 2016, corresponding to
             integrated luminosities of 3.5 fb-1 and 33.5 fb-1
             respectively. Invariant mass and angular distributions are
             compared to background predictions and no significant
             deviation is observed. For resonance searches, a new method
             for fitting the background component of the invariant mass
             distribution is employed. The data set is then used to set
             upper limits at a 95% confidence level on a range of new
             physics scenarios. Excited quarks with masses below 6.0 TeV
             are excluded, and limits are set on quantum black holes,
             heavy W′ bosons, W∗ bosons, and a range of masses and
             couplings in a Z′ dark matter mediator model.
             Model-independent limits on signals with a Gaussian shape
             are also set, using a new approach allowing factorization of
             physics and detector effects. From the angular
             distributions, a scale of new physics in contact interaction
             models is excluded for scenarios with either constructive or
             destructive interference. These results represent a
             substantial improvement over those obtained previously with
             lower integrated luminosity.},
   Doi = {10.1103/PhysRevD.96.052004},
   Key = {fds356740}
}

@article{fds356775,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O},
   Title = {Search for new phenomena in dijet mass and angular
             distributions from pp collisions at √s=13 TeV with the
             ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {754},
   Pages = {302-322},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.01.032},
   Abstract = {This Letter describes a model-agnostic search for pairs of
             jets (dijets) produced by resonant and non-resonant
             phenomena beyond the Standard Model in 3.6 fb−1 of
             proton–proton collisions with a centre-of-mass energy of
             s=13 TeV recorded by the ATLAS detector at the Large Hadron
             Collider. The distribution of the invariant mass of the two
             leading jets is examined for local excesses above a
             data-derived estimate of the smoothly falling prediction of
             the Standard Model. The data are also compared to a Monte
             Carlo simulation of Standard Model angular distributions
             derived from the rapidity of the two jets. No evidence of
             anomalous phenomena is observed in the data, which are used
             to exclude, at 95% CL, quantum black holes with threshold
             masses below 8.3 TeV, 8.1 TeV, or 5.1 TeV in three different
             benchmark scenarios; resonance masses below 5.2 TeV for
             excited quarks, 2.6 TeV in a W′ model, a range of masses
             starting from mZ′=1.5 TeV and couplings from gq=0.2 in a
             Z′ model; and contact interactions with a compositeness
             scale below 12.0 TeV and 17.5 TeV respectively for
             destructive and constructive interference between the new
             interaction and QCD processes. These results significantly
             extend the ATLAS limits obtained from 8 TeV data.
             Gaussian-shaped contributions to the mass distribution are
             also excluded if the effective cross-section exceeds values
             ranging from approximately 50–300 fb for masses below 2
             TeV to 2–20 fb for masses above 4 TeV.},
   Doi = {10.1016/j.physletb.2016.01.032},
   Key = {fds356775}
}

@article{fds347493,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
             H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
             L and Adams, DL and Adelman, J and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
             D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa,
             JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti,
             M and De Mendizabal and JB and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
             J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
             Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castelli,
             A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich,
             LC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
             A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro,
             A},
   Title = {Search for new phenomena in events containing a same-flavour
             opposite-sign dilepton pair, jets, and large missing
             transverse momentum in [Formula: see text] [Formula: see
             text][Formula: see text] collisions with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {3},
   Pages = {144},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4700-5},
   Abstract = {Two searches for new phenomena in final states containing a
             same-flavour opposite-sign lepton (electron or muon) pair,
             jets, and large missing transverse momentum are presented.
             These searches make use of proton-proton collision data,
             collected during 2015 and 2016 at a centre-of-mass energy
             [Formula: see text] [Formula: see text] by the ATLAS
             detector at the large hadron collider, which correspond to
             an integrated luminosity of [Formula: see text]. Both
             searches target the pair production of supersymmetric
             particles, squarks or gluinos, which decay to final states
             containing a same-flavour opposite-sign lepton pair via one
             of two mechanisms: a leptonically decaying <i>Z</i> boson in
             the final state, leading to a peak in the dilepton
             invariant-mass distribution around the <i>Z</i> boson mass;
             and decays of neutralinos (e.g. [Formula: see text]),
             yielding a kinematic endpoint in the dilepton invariant-mass
             spectrum. The data are found to be consistent with the
             Standard Model expectation. Results are interpreted in
             simplified models of gluino-pair (squark-pair) production,
             and provide sensitivity to gluinos (squarks) with masses as
             large as 1.70 [Formula: see text] (980 [Formula: see
             text]).},
   Doi = {10.1140/epjc/s10052-017-4700-5},
   Key = {fds347493}
}

@article{fds321125,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Search for new phenomena in events with a photon and missing
             transverse momentum in pp collisions at √s = 13 TeV with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {6},
   Pages = {1-41},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2016)059},
   Abstract = {Results of a search for new phenomena in events with an
             energetic photon and large missing transverse momentum with
             the ATLAS experiment at the Large Hadron Collider are
             reported. The data were collected in proton-proton
             collisions at a centre-of-mass energy of 13 TeV and
             correspond to an integrated luminosity of 3.2 fb−1. The
             observed data are in agreement with the Standard Model
             expectations. Exclusion limits are presented in models of
             new phenomena including pair production of dark matter
             candidates or large extra spatial dimensions. In a
             simplified model of dark matter and an axial-vector
             mediator, the search excludes mediator masses below 710 GeV
             for dark matter candidate masses below 150 GeV. In an
             effective theory of dark matter production, values of the
             suppression scale M∗ up to 570 GeV are excluded and the
             effect of truncation for various coupling values is
             reported. For the ADD large extra spatial dimension model
             the search places more stringent limits than earlier
             searches in the same event topology, excluding MD up to
             about 2.3 (2.8) TeV for two (six) additional spatial
             dimensions; the limits are reduced by 20-40% depending on
             the number of additional spatial dimensions when applying a
             truncation procedure.},
   Doi = {10.1007/JHEP06(2016)059},
   Key = {fds321125}
}

@article{fds310327,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for new phenomena in events with a photon and missing
             transverse momentum in pp collisions at √s =8 TeV with the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.012008},
   Abstract = {Results of a search for new phenomena in events with an
             energetic photon and large missing transverse momentum with
             the ATLAS experiment at the LHC are reported. Data were
             collected in proton-proton collisions at a center-of-mass
             energy of 8 TeV and correspond to an integrated luminosity
             of 20.3 fb-1. The observed data are well described by the
             expected Standard Model backgrounds. The expected (observed)
             upper limit on the fiducial cross section for the production
             of events with a photon and large missing transverse
             momentum is 6.1 (5.3) fb at 95% confidence level. Exclusion
             limits are presented on models of new phenomena with large
             extra spatial dimensions, supersymmetric quarks, and direct
             pair production of dark-matter candidates.},
   Doi = {10.1103/PhysRevD.91.012008},
   Key = {fds310327}
}

@article{fds315361,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
             A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP},
   Title = {Search for new phenomena in events with at least three
             photons collected in pp collisions at [Formula: see
             text] = 8 TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {4},
   Pages = {210},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4034-8},
   Abstract = {Results of a search for new phenomena in events with at
             least three photons are reported. Data from proton-proton
             collisions at a centre-of-mass energy of 8 TeV,
             corresponding to an integrated luminosity of 20.3
             fb[Formula: see text], were collected with the ATLAS
             detector at the LHC. The observed data are well described by
             the Standard Model. Limits at the 95 % confidence level on
             new phenomena are presented based on the rate of events in
             an inclusive signal region and a restricted signal region
             targeting the rare decay [Formula: see text], as well as
             di-photon and tri-photon resonance searches. For a Standard
             Model Higgs boson decaying to four photons via a pair of
             intermediate pseudoscalar particles (<i>a</i>), limits are
             found to be [Formula: see text] for 10 GeV [Formula: see
             text] 62 GeV. Limits are also presented for Higgs boson-like
             scalars (<i>H</i>) for [Formula: see text] 125 GeV, and for
             a [Formula: see text] decaying to three photons via
             [Formula: see text]. Additionally, the observed limit on the
             branching ratio of the <i>Z</i> boson decay to three photons
             is found to be BR[Formula: see text], a result five times
             stronger than the previous result from LEP.},
   Doi = {10.1140/epjc/s10052-016-4034-8},
   Key = {fds315361}
}

@article{fds356634,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Search for new phenomena in events with same-charge leptons
             and b-jets in pp collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {12},
   Year = {2018},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2018)039},
   Abstract = {A search for new phenomena in events with two same-charge
             leptons or three leptons and jets identified as originating
             from b-quarks in a data sample of 36.1 fb−1 of pp
             collisions at s=13 TeV recorded by the ATLAS detector at the
             Large Hadron Collider is reported. No significant excess is
             found and limits are set on vector-like quark,
             four-top-quark, and same-sign top-quark pair production. The
             observed (expected) 95% CL mass limits for a vector-like T-
             and B-quark singlet are mT > 0.98 (0.99) TeV and mB > 1.00
             (1.01) TeV respectively. Limits on the production of the
             vector-like T5/3-quark are also derived considering both
             pair and single production; in the former case the lower
             limit on the mass of the T5/3-quark is (expected to be) 1.19
             (1.21) TeV. The Standard Model four-top-quark production
             cross-section upper limit is (expected to be) 69 (29) fb.
             Constraints are also set on exotic four-top-quark production
             models. Finally, limits are set on same-sign top-quark pair
             production. The upper limit on uu → tt production is
             (expected to be) 89 (59) fb for a mediator mass of 1 TeV,
             and a dark-matter interpretation is also derived, excluding
             a mediator of 3 TeV with a dark-sector coupling of 1.0 and a
             coupling to ordinary matter above 0.31.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP12(2018)039},
   Key = {fds356634}
}

@article{fds307613,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for new phenomena in events with three charged
             leptons at √s=7 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.052002},
   Abstract = {A generic search for anomalous production of events with at
             least three charged leptons is presented. The search uses a
             pp-collision data sample at a center-of-mass energy of
             √s=7 TeV corresponding to 4.6 fb-1 of integrated
             luminosity collected in 2011 by the ATLAS detector at the
             CERN Large Hadron Collider. Events are required to contain
             at least two electrons or muons, while the third lepton may
             either be an additional electron or muon, or a hadronically
             decaying tau lepton. Events are categorized by the presence
             or absence of a reconstructed tau-lepton or Z-boson
             candidate decaying to leptons. No significant excess above
             backgrounds expected from Standard Model processes is
             observed. Results are presented as upper limits on event
             yields from non-Standard-Model processes producing at least
             three prompt, isolated leptons, given as functions of lower
             bounds on several kinematic variables. Fiducial efficiencies
             for model testing are also provided. The use of the results
             is illustrated by setting upper limits on the production of
             doubly charged Higgs bosons decaying to same-sign lepton
             pairs.},
   Doi = {10.1103/PhysRevD.87.052002},
   Key = {fds307613}
}

@article{fds317298,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
             M},
   Title = {Search for new phenomena in events with three or more
             charged leptons in pp collisions at √s=8 TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2015)138},
   Abstract = {Abstract: A generic search for anomalous production of
             events with at least three charged leptons is presented. The
             data sample consists of pp collisions at √s=8 TeV
             collected in 2012 by the ATLAS experiment at the CERN Large
             Hadron Collider, and corresponds to an integrated luminosity
             of 20.3 fb−1. Events are required to have at least three
             selected lepton candidates, at least two of which must be
             electrons or muons, while the third may be a hadronically
             decaying tau. Selected events are categorized based on their
             lepton flavour content and signal regions are constructed
             using several kinematic variables of interest. No
             significant deviations from Standard Model predictions are
             observed. Model-independent upper limits on contributions
             from beyond the Standard Model phenomena are provided for
             each signal region, along with prescription to re-interpret
             the limits for any model. Constraints are also placed on
             models predicting doubly charged Higgs bosons and excited
             leptons. For doubly charged Higgs bosons decaying to eτ or
             μτ, lower limits on the mass are set at 400 GeV at 95%
             confidence level. For excited leptons, constraints are
             provided as functions of both the mass of the excited state
             and the compositeness scale Λ, with the strongest mass
             constraints arising in regions where the mass equals Λ. In
             such scenarios, lower mass limits are set at 3.0 TeV for
             excited electrons and muons, 2.5 TeV for excited taus, and
             1.6 TeV for every excited-neutrino flavour.},
   Doi = {10.1007/JHEP08(2015)138},
   Key = {fds317298}
}

@article{fds356104,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
             C},
   Title = {Search for new phenomena in events with two opposite-charge
             leptons, jets and missing transverse momentum in pp
             collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {4},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2021)165},
   Abstract = {The results of a search for direct pair production of top
             squarks and for dark matter in events with two
             opposite-charge leptons (electrons or muons), jets and
             missing transverse momentum are reported, using 139 fb−1
             of integrated luminosity from proton-proton collisions at s
             = 13 TeV, collected by the ATLAS detector at the Large
             Hadron Collider during Run 2 (2015–2018). This search
             considers the pair production of top squarks and is
             sensitive across a wide range of mass differences between
             the top squark and the lightest neutralino. Additionally,
             spin-0 mediator dark-matter models are considered, in which
             the mediator is produced in association with a pair of top
             quarks. The mediator subsequently decays to a pair of
             dark-matter particles. No significant excess of events is
             observed above the Standard Model background, and limits are
             set at 95% confidence level. The results exclude top squark
             masses up to about 1 TeV, and masses of the lightest
             neutralino up to about 500 GeV. Limits on dark-matter
             production are set for scalar (pseudoscalar) mediator masses
             up to about 250 (300) GeV. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP04(2021)165},
   Key = {fds356104}
}

@article{fds307809,
   Author = {Kotwal, AV and Collaboration, CDF},
   Title = {Search for new phenomena in events with two Z bosons and
             missing transverse momentum in ppbar collisions at
             sqrt(s)=1.96 TeV},
   Journal = {Phys. Rev. D},
   Volume = {85},
   Number = {1},
   Pages = {011104(R)},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.011104},
   Abstract = {We present a search for new phenomena in events with two
             reconstructed Z bosons and large missing transverse
             momentum, sensitive to processes pp̄→X 2X 2→ZZX 1X 1,
             where X 2 is an unstable particle decaying as X 2→ ZX 1
             and X 1 is undetected. The particles X 1 and X 2 may be,
             among other possibilities, fourth-generation neutrinos or
             supersymmetric particles. We study the final state in which
             one Z boson decays to two charged leptons and the second
             decays hadronically. In data corresponding to an integrated
             luminosity of 4.2fb -1 from proton-antiproton collisions
             recorded by the CDF II detector at the Tevatron, with
             center-of-mass energy of 1.96 TeV, we find agreement between
             data and standard-model backgrounds. We calculate 95%
             confidence level upper limits on the cross section of the
             process pp̄→X 2X 2→ZZX 1X 1 ranging from 50 fb to 1 pb,
             depending on the masses of X 1 and X 2. © 2012 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.85.011104},
   Key = {fds307809}
}

@article{fds310324,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
             C},
   Title = {Search for new phenomena in final states with an energetic
             jet and large missing transverse momentum in pp
             collisions at [Formula: see text]TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {299},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3517-3},
   Abstract = {Results of a search for new phenomena in final states with
             an energetic jet and large missing transverse momentum are
             reported. The search uses 20.3 fb[Formula: see text] of
             [Formula: see text] TeV data collected in 2012 with the
             ATLAS detector at the LHC. Events are required to have at
             least one jet with [Formula: see text] GeV and no leptons.
             Nine signal regions are considered with increasing missing
             transverse momentum requirements between [Formula: see
             text] GeV and [Formula: see text] GeV. Good agreement is
             observed between the number of events in data and Standard
             Model expectations. The results are translated into
             exclusion limits on models with either large extra spatial
             dimensions, pair production of weakly interacting dark
             matter candidates, or production of very light gravitinos in
             a gauge-mediated supersymmetric model. In addition, limits
             on the production of an invisibly decaying Higgs-like boson
             leading to similar topologies in the final state are
             presented.},
   Doi = {10.1140/epjc/s10052-015-3517-3},
   Key = {fds310324}
}

@article{fds321110,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for new phenomena in final states with an energetic
             jet and large missing transverse momentum in pp collisions
             at s =13 TeV using the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.032005},
   Abstract = {Results of a search for new phenomena in final states with
             an energetic jet and large missing transverse momentum are
             reported. The search uses proton-proton collision data
             corresponding to an integrated luminosity of 3.2 fb-1 at
             s=13 TeV collected in 2015 with the ATLAS detector at the
             Large Hadron Collider. Events are required to have at least
             one jet with a transverse momentum above 250 GeV and no
             leptons. Several signal regions are considered with
             increasing missing-transverse-momentum requirements between
             ETmiss>250 GeV and ETmiss>700 GeV. Good agreement is
             observed between the number of events in data and Standard
             Model predictions. The results are translated into exclusion
             limits in models with large extra spatial dimensions, pair
             production of weakly interacting dark-matter candidates, and
             the production of supersymmetric particles in several
             compressed scenarios.},
   Doi = {10.1103/PhysRevD.94.032005},
   Key = {fds321110}
}

@article{fds312133,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Search for new phenomena in final states with large jet
             multiplicities and missing transverse momentum at √s = 8
             TeV proton-proton collisions using the ATLAS
             experiment},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2013)130},
   Abstract = {A search is presented for new particles decaying to large
             numbers (7 or more) of jets, with missing transverse
             momentum and no isolated electrons or muons. This analysis
             uses 20:3 fb-1 of pp collision data at √s = 8 TeV
             collected by the ATLAS experiment at the Large Hadron
             Collider. The sensitivity of the search is enhanced by
             considering the number of b-tagged jets and the scalar sum
             of masses of large-radius jets in an event. No evidence is
             found for physics beyond the Standard Model. The results are
             interpreted in the context of various simplified
             supersymmetry-inspired models where gluinos are pair
             produced, as well as an mSUGRA/CMSSM model. © SISSA
             2013.},
   Doi = {10.1007/JHEP10(2013)130},
   Key = {fds312133}
}

@article{fds320777,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for new phenomena in final states with large jet
             multiplicities and missing transverse momentum using √s =
             7 TeV pp collisions with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2011},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP11(2011)099},
   Abstract = {Results are presented of a search for any particle(s)
             decaying to six or more jets in association with missing
             transverse momentum. The search is performed using
             1.34fb−1 of √s = 7 TeV proton-proton collisions recorded
             by the ATLAS detector during 2011. Data-driven techniques
             are used to determine the backgrounds in kinematic regions
             that require at least six, seven or eight jets, well beyond
             the multiplicities required in previous analyses. No
             evidence is found for physics beyond the Standard Model. The
             results are interpreted in the context of a supersymmetry
             model (MSUGRA/CMSSM) where they extend previous
             constraints.},
   Doi = {10.1007/JHEP11(2011)099},
   Key = {fds320777}
}

@article{fds315359,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A},
   Title = {Search for new phenomena in final states with large jet
             multiplicities and missing transverse momentum with ATLAS
             using √s=13 TeV proton–proton collisions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {757},
   Pages = {334-355},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {June},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.04.005},
   Abstract = {Results are reported of a search for new phenomena, such as
             supersymmetric particle production, that could be observed
             in high-energy proton–proton collisions. Events with large
             numbers of jets, together with missing transverse momentum
             from unobserved particles, are selected. The data analysed
             were recorded by the ATLAS experiment during 2015 using the
             13 TeV centre-of-mass proton–proton collisions at the
             Large Hadron Collider, and correspond to an integrated
             luminosity of 3.2 fb−1. The search selected events with
             various jet multiplicities from ≥7 to ≥10 jets, and with
             various b-jet multiplicity requirements to enhance
             sensitivity. No excess above Standard Model expectations is
             observed. The results are interpreted within two
             supersymmetry models, where gluino masses up to 1400 GeV are
             excluded at 95% confidence level, significantly extending
             previous limits.},
   Doi = {10.1016/j.physletb.2016.04.005},
   Key = {fds315359}
}

@article{fds359673,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin,
             RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Backman, F and Badea, A and Bagnaia, P and Bahrasemani, H and Bailey, AJ and Bailey,
             VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends,
             KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau,
             T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov, VA and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos,
             P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun,
             D and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
             Kuutmann, E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer,
             J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia
             Bylund, O and Bethke, S and Betti, A and Bevan, AJ and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biesuz, NV and Biglietti,
             M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
             JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner,
             L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr,
             JTP and Burton, CD and Burzynski, JC and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo
             Vazquez, CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba,
             LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capua, M and Carbone, A and Cardarelli, R and Cardillo, F and Carducci, G and Carli,
             T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carter, JWS and Carter, TM and Casadei, D and Casado,
             MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia,
             L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
             JR and Cattai, A and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chau, CC and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, CL and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, YS and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark,
             A and Clark, PJ and Clavijo Columbie and JM and Clawson, SE and Clement, C and Clissa, L and Coadou, Y},
   Title = {Search for New Phenomena in Final States with Two Leptons
             and One or No b-Tagged Jets at sqrt[s]=13  TeV Using the
             ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {127},
   Number = {14},
   Pages = {141801},
   Year = {2021},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.127.141801},
   Abstract = {A search for new phenomena is presented in final states with
             two leptons and one or no b-tagged jets. The event selection
             requires the two leptons to have opposite charge, the same
             flavor (electrons or muons), and a large invariant mass. The
             analysis is based on the full run-2 proton-proton collision
             dataset recorded at a center-of-mass energy of
             sqrt[s]=13  TeV by the ATLAS experiment at the LHC,
             corresponding to an integrated luminosity of
             139  fb^{-1}. No significant deviation from the expected
             background is observed in the data. Inspired by the B-meson
             decay anomalies, a four-fermion contact interaction between
             two quarks (b, s) and two leptons (ee or μμ) is used as a
             benchmark signal model, which is characterized by the energy
             scale and coupling, Λ and g_{*}, respectively. Contact
             interactions with Λ/g_{*} lower than 2.0 (2.4) TeV are
             excluded for electrons (muons) at the 95% confidence level,
             still far below the value that is favored by the B-meson
             decay anomalies. Model-independent limits are set as a
             function of the minimum dilepton invariant mass, which allow
             the results to be reinterpreted in various signal
             scenarios.},
   Doi = {10.1103/physrevlett.127.141801},
   Key = {fds359673}
}

@article{fds356712,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for new phenomena in high-mass diphoton final states
             using 37 fb−1 of proton–proton collisions
             collected at s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {775},
   Pages = {105-125},
   Year = {2017},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2017.10.039},
   Abstract = {Searches for new phenomena in high-mass diphoton final
             states with the ATLAS experiment at the LHC are presented.
             The analysis is based on pp collision data corresponding to
             an integrated luminosity of 36.7 fb−1 at a centre-of-mass
             energy s=13 TeV recorded in 2015 and 2016. Searches are
             performed for resonances with spin 0, as predicted by
             theories with an extended Higgs sector, and for resonances
             with spin 2, using a warped extra-dimension model as a
             benchmark model, as well as for non-resonant signals,
             assuming a large extra-dimension scenario. No significant
             deviation from the Standard Model is observed. Upper limits
             are placed on the production cross section times branching
             ratio to two photons as a function of the resonance mass. In
             addition, lower limits are set on the ultraviolet cutoff
             scale in the large extra-dimensions model.},
   Doi = {10.1016/j.physletb.2017.10.039},
   Key = {fds356712}
}

@article{fds347465,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
             C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
             AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz,
             T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair,
             RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau,
             JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni,
             A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
             MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard,
             CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher,
             V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cai, H and Cairo, VM and Cakir, O and Calace,
             N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
             S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini,
             I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
             YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
             YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
   Title = {Search for new phenomena in high-mass final states with a
             photon and a jet from pp collisions at s = 13 TeV with the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {2},
   Pages = {102},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-5553-2},
   Abstract = {A search is performed for new phenomena in events having a
             photon with high transverse momentum and a jet collected in
             36.7 fb - 1 of proton-proton collisions at a centre-of-mass
             energy of s = 13 TeV recorded with the ATLAS detector at
             the Large Hadron Collider. The invariant mass distribution
             of the leading photon and jet is examined to look for the
             resonant production of new particles or the presence of new
             high-mass states beyond the Standard Model. No significant
             deviation from the background-only hypothesis is observed
             and cross-section limits for generic Gaussian-shaped
             resonances are extracted. Excited quarks hypothesized in
             quark compositeness models and high-mass states predicted in
             quantum black hole models with extra dimensions are also
             examined in the analysis. The observed data exclude, at 95%
             confidence level, the mass range below 5.3 TeV for excited
             quarks and 7.1 TeV (4.4 TeV) for quantum black holes in
             the Arkani-Hamed-Dimopoulos-Dvali (Randall-Sundrum) model
             with six (one) extra dimensions.},
   Doi = {10.1140/epjc/s10052-018-5553-2},
   Key = {fds347465}
}

@article{fds307553,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Search for new phenomena in photon + jet events collected in
             proton-proton collisions at √s = 8 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {728},
   Number = {1},
   Pages = {562-578},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.12.029},
   Abstract = {This Letter describes a model-independent search for the
             production of new resonances in photon + jet (γ + jet)
             events using 20 fb-1 of proton-proton LHC data recorded with
             the ATLAS detector at a centre-of-mass energy of √s = 8
             TeV. The γ + jet mass distribution is compared to a
             background model fit from data; no significant deviation
             from the background-only hypothesis is found. Limits are set
             at 95% credibility level on generic Gaussian-shaped signals
             and two benchmark phenomena beyond the Standard Model:
             non-thermal quantum black holes and excited quarks.
             Non-thermal quantum black holes are excluded below masses of
             4.6 TeV and excited quarks are excluded below masses of 3.5
             TeV. © 2013 The Authors. Published by Elsevier
             B.V.},
   Doi = {10.1016/j.physletb.2013.12.029},
   Key = {fds307553}
}

@article{fds310296,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for new phenomena in the dijet mass distribution
             using pp collision data at √s =8 TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.052007},
   Abstract = {Dijet events produced in LHC proton-proton collisions at a
             center-of-mass energy s=8 TeV are studied with the ATLAS
             detector using the full 2012 data set, with an integrated
             luminosity of 20.3 fb-1. Dijet masses up to about 4.5 TeV
             are probed. No resonancelike features are observed in the
             dijet mass spectrum. Limits on the cross section times
             acceptance are set at the 95% credibility level for various
             hypotheses of new phenomena in terms of mass or energy
             scale, as appropriate. This analysis excludes excited quarks
             with a mass below 4.06 TeV, color-octet scalars with a mass
             below 2.70 TeV, heavy W′ bosons with a mass below 2.45
             TeV, chiral W∗ bosons with a mass below 1.75 TeV, and
             quantum black holes with six extra space-time dimensions
             with threshold mass below 5.66 TeV.},
   Doi = {10.1103/PhysRevD.91.052007},
   Key = {fds310296}
}

@article{fds307636,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arika, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, R and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
             Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Urban, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Armadans,
             RC and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido,
             MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez,
             VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas,
             CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M},
   Title = {Search for new phenomena in the WW → |v|′v′ final
             state in pp collisions at √s=7 TeV with the ATLAS
             detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {718},
   Number = {3},
   Pages = {860-878},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.11.040},
   Abstract = {This Letter reports a search for a heavy particle that
             decays to WW using events produced in pp collisions at
             s=7TeV. The data were recorded in 2011 by the ATLAS detector
             and correspond to an integrated luminosity of 4.7 fb-1.
             WW→ℓνℓ'ν'(ℓ, ℓ'=e or μ) final states are
             considered and the distribution of the transverse mass of
             the WW candidates is found to be consistent with Standard
             Model expectations. Upper limits on the production cross
             section times branching ratio into W boson pairs are set for
             Randall-Sundrum and bulk Randall-Sundrum gravitons, which
             result in observed 95% CL lower limits on the masses of the
             two particles of 1.23 TeV and 0.84 TeV, respectively. ©
             2012 CERN.},
   Doi = {10.1016/j.physletb.2012.11.040},
   Key = {fds307636}
}

@article{fds307715,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
             G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
             M and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius,
             C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall,
             J},
   Title = {Search for new phenomena in tt events with large missing
             transverse momentum in proton-proton collisions at sqrt[s] =
             7 TeV with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {4},
   Pages = {041805},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.108.041805},
   Abstract = {A search for new phenomena in tt events with large missing
             transverse momentum in proton-proton collisions at a
             center-of-mass energy of 7 TeV is presented. The measurement
             is based on 1.04 fb(-1) of data collected with the ATLAS
             detector at the LHC. Contributions to this final state may
             arise from a number of standard model extensions. The
             results are interpreted in terms of a model where new
             top-quark partners are pair produced and each decay to an
             on-shell top (or antitop) quark and a long-lived undetected
             neutral particle. The data are found to be consistent with
             standard model expectations. A limit at 95% confidence level
             is set excluding a cross section times branching ratio of
             1.1 pb for a top-partner mass of 420 GeV and a neutral
             particle mass less than 10 GeV. In a model of exotic fourth
             generation quarks, top-partner masses are excluded up to 420
             GeV and neutral particle masses up to 140
             GeV.},
   Doi = {10.1103/physrevlett.108.041805},
   Key = {fds307715}
}

@article{fds376248,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
             J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
             GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
             Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
             C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
             M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
             SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena,
             E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis,
             K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balakrishnan, V and Balasubramanian,
             R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio,
             EL and Barberis, D and Barbero, M and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco
             Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau,
             T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
             L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry,
             T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Biryukov, S and Bisanz, T and Bisceglie, E and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac,
             D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold,
             T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély,
             AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov,
             G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruni,
             A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr,
             JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev, AR and Cabrera
             Urbán, S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo,
             VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson,
             EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter,
             JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cepaitis, V and Cerny, K and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli,
             A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chan,
             J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
             Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
             J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
             A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM},
   Title = {Search for New Phenomena in Two-Body Invariant Mass
             Distributions Using Unsupervised Machine Learning for
             Anomaly Detection at sqrt[s]=13  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {132},
   Number = {8},
   Pages = {081801},
   Year = {2024},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.132.081801},
   Abstract = {Searches for new resonances are performed using an
             unsupervised anomaly-detection technique. Events with at
             least one electron or muon are selected from
             140  fb^{-1} of pp collisions at sqrt[s]=13  TeV
             recorded by ATLAS at the Large Hadron Collider. The approach
             involves training an autoencoder on data, and subsequently
             defining anomalous regions based on the reconstruction loss
             of the decoder. Studies focus on nine invariant mass spectra
             that contain pairs of objects consisting of one light jet or
             b jet and either one lepton (e,μ), photon, or second light
             jet or b jet in the anomalous regions. No significant
             deviations from the background hypotheses are observed.
             Limits on contributions from generic Gaussian signals with
             various widths of the resonance mass are obtained for nine
             invariant masses in the anomalous regions.},
   Doi = {10.1103/physrevlett.132.081801},
   Key = {fds376248}
}

@article{fds347478,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and AlconadaVerzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and AlvarezGonzalez,
             B and ÁlvarezPiqueras, D and Alviggi, MG and Amadio, BT and AmaralCoutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor
             DosSantos, SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and AraujoFerraz, V and Pereira, RA and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov,
             A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
             M and Baker, OK and Bakker, PJ and Gupta, DB and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee,
             S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
             A and Barone, G and Barr, AJ and BarrancoNavarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary,
             O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and BenharNoccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertram, IA and Bertsche, C and Besjes, GJ and BessidskaiaBylund, O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
             NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini,
             C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black,
             JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boerner,
             D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona,
             M and Bonilla, JSB and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and BossioSola, JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt,
             A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
             DL and Bristow, TM and Britton, D and Britzger, D and Brock, I and Brock,
             R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman deRenstrom, PA and Bruncko, D and Bruni,
             A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
             MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard,
             CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and CabreraUrbán, S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and CalventeLopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and CamachoToro, R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and CanoBret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and CastilloGimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and CerdaAlberich, L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             DC and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen,
             SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui ElMoursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară,
             IA and Ciocio, A and Cirotto, F and Citron, ZH},
   Title = {Search for new phenomena using the invariant mass
             distribution of same-flavour opposite-sign dilepton pairs in
             events with missing transverse momentum in s=13  
             Tepp collisions with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {8},
   Pages = {625},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-6081-9},
   Abstract = {A search for new phenomena in final states containing an
             e+e- or μ+μ- pair, jets, and large missing transverse
             momentum is presented. This analysis makes use of
             proton-proton collision data with an integrated luminosity
             of 36.1fb-1 , collected during 2015 and 2016 at a
             centre-of-mass energy s=13TeV with the ATLAS detector at the
             Large Hadron Collider. The search targets the pair
             production of supersymmetric coloured particles (squarks or
             gluinos) and their decays into final states containing an
             e+e- or μ+μ- pair and the lightest neutralino ( χ~10 )
             via one of two next-to-lightest neutralino ( χ~20 ) decay
             mechanisms: χ~20→Zχ~10 , where the <i>Z</i> boson decays
             leptonically leading to a peak in the dilepton invariant
             mass distribution around the <i>Z</i> boson mass; and
             χ~20→ℓ+ℓ-χ~10 with no intermediate ℓ+ℓ-
             resonance, yielding a kinematic endpoint in the dilepton
             invariant mass spectrum. The data are found to be consistent
             with the Standard Model expectation. Results are interpreted
             using simplified models, and exclude gluinos and squarks
             with masses as large as 1.85 and 1.3  Te at 95% confidence
             level, respectively.},
   Doi = {10.1140/epjc/s10052-018-6081-9},
   Key = {fds347478}
}

@article{fds356715,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Search for new phenomena with large jet multiplicities and
             missing transverse momentum using large-radius jets and
             flavour-tagging at ATLAS in 13 TeV pp collisions},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {12},
   Year = {2017},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2017)034},
   Abstract = {A search is presented for particles that decay producing a
             large jet multiplicity and invisible particles. The event
             selection applies a veto on the presence of isolated
             electrons or muons and additional requirements on the number
             of b-tagged jets and the scalar sum of masses of
             large-radius jets. Having explored the full ATLAS 2015-2016
             dataset of LHC proton-proton collisions at s=13 TeV, which
             corresponds to 36.1 fb−1 of integrated luminosity, no
             evidence is found for physics beyond the Standard Model. The
             results are interpreted in the context of simplified models
             inspired by R-parity-conserving and R-parity-violating
             supersymmetry, where gluinos are pair-produced. More generic
             models within the phenomenological minimal supersymmetric
             Standard Model are also considered.},
   Doi = {10.1007/JHEP12(2017)034},
   Key = {fds356715}
}

@article{fds356776,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Search for new phenomena with photon+jet events in
             proton-proton collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {3},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2016)041},
   Abstract = {Abstract: A search is performed for the production of
             high-mass resonances decaying into a photon and a jet in 3.2
             fb−1of proton-proton collisions at a centre-of-mass energy
             of (Formula presented.) TeV collected by the ATLAS detector
             at the Large Hadron Collider. Selected events have an
             isolated photon and a jet, each with transverse momentum
             above 150 GeV. No significant deviation of the γ+jet
             invariant mass distribution from the background-only
             hypothesis is found. Limits are set at 95% confidence level
             on the cross sections of generic Gaussian-shaped signals and
             of a few benchmark phenomena beyond the Standard Model:
             excited quarks with vector-like couplings to the Standard
             Model particles, and non-thermal quantum black holes in two
             models of extra spatial dimensions. The minimum excluded
             visible cross sections for Gaussian-shaped resonances with
             width-to-mass ratios of 2% decrease from about 6 fb for a
             mass of 1.5 TeV to about 0.8 fb for a mass of 5 TeV. The
             minimum excluded visible cross sections for Gaussian-shaped
             resonances with width-to-mass ratios of 15% decrease from
             about 50 fb for a mass of 1.5 TeV to about 1.0 fb for a mass
             of 5 TeV. Excited quarks are excluded below masses of 4.4
             TeV, and non-thermal quantum black holes are excluded below
             masses of 3.8 (6.2) TeV for Randall-Sundrum
             (Arkani-Hamed-Dimopoulous-Dvali) models with one (six) extra
             dimensions.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP03(2016)041},
   Key = {fds356776}
}

@article{fds307863,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Search for new phenomena with the monojet and missing
             transverse momentum signature using the ATLAS detector in
             s=7TeV proton-proton collisions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {4},
   Pages = {294-312},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.10.006},
   Abstract = {A search for new phenomena in events featuring a high energy
             jet and large missing transverse momentum in proton-proton
             collisions at s=7TeV is presented using a dataset
             corresponding to an integrated luminosity of 33 pb-1
             recorded with the ATLAS detector at the Large Hadron
             Collider. The number of observed events is consistent with
             the Standard Model prediction. This result is interpreted in
             terms of limits on a model of Large Extra Dimensions. ©
             2011 CERN.},
   Doi = {10.1016/j.physletb.2011.10.006},
   Key = {fds307863}
}

@article{fds356105,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
             C},
   Title = {Search for new phenomena with top quark pairs in final
             states with one lepton, jets, and missing transverse
             momentum in pp collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {4},
   Year = {2021},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2021)174},
   Abstract = {A search for new phenomena with top quark pairs in final
             states with one isolated electron or muon, multiple jets,
             and large missing transverse momentum is performed. Signal
             regions are designed to search for two-, three-, and
             four-body decays of the directly pair-produced
             supersymmetric partner of the top quark (stop). Additional
             signal regions are designed specifically to search for
             spin-0 mediators that are produced in association with a
             pair of top quarks and decay into a pair of dark-matter
             particles. The search is performed using the Large Hadron
             Collider proton-proton collision dataset at a centre-of-mass
             energy of s = 13 TeV recorded by the ATLAS detector from
             2015 to 2018, corresponding to an integrated luminosity of
             139 fb−1. No significant excess above the Standard Model
             background is observed, and limits at 95% confidence level
             are set in the stop-neutralino mass plane and as a function
             of the mediator mass or the dark-matter particle mass. Stops
             are excluded up to 1200 GeV (710 GeV) in the two-body
             (three-body) decay scenario. In the four-body scenario stops
             up to 640 GeV are excluded for a stop-neutralino mass
             difference of 60 GeV. Scalar and pseudoscalar dark-matter
             mediators are excluded up to 200 GeV when the coupling
             strengths of the mediator to Standard Model and dark-matter
             particles are both equal to one and when the mass of the
             dark-matter particle is 1 GeV. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP04(2021)174},
   Key = {fds356105}
}

@article{fds307835,
   Author = {Aaltonen, TEA},
   Title = {Search for New Physics in High ${p}_{T}$ Like-Sign Dilepton
             Events at {CDF II}},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {18},
   Pages = {181801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.181801},
   Abstract = {We present a search for new physics in events with two high
             pT leptons of the same electric charge, using data with an
             integrated luminosity of 6.1 fb(-1). The observed data are
             consistent with standard model predictions. We set 95% C.L.
             lower limits on the mass of doubly charged scalars decaying
             to like-sign dileptons, m(H±±) > 190-245 GeV/c(2),
             assuming 100% BR to ee, μμ or eμ.},
   Doi = {10.1103/PhysRevLett.107.181801},
   Key = {fds307835}
}

@article{fds308050,
   Author = {Aaltonen, and T, and others},
   Title = {Search for new physics in high mass electron-positron events
             in $p \bar{p}$ collisions at $\sqrt{s}$ =
             1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {17},
   Pages = {171802},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.99.171802},
   Abstract = {We report the results of a search for a narrow resonance in
             electron-positron events in the invariant mass range of
             150--950 GeV/c2 using 1.3 fb-1 of p[overline p] collision
             data at sqrt(s)=1.96 TeV collected by the CDF II detector at
             Fermilab. No significant evidence of such a resonance is
             observed and we interpret the results to exclude the
             standard-model-like Z[prime] with a mass below 923 GeV/c2
             and the Randall-Sundrum graviton with a mass below 807
             GeV/c2 for k/[overline M]pl=0.1, both at the 95\% confidence
             level. Combining with diphoton data excludes the
             Randall-Sundrum graviton for masses below 889 GeV/c2 for
             k/[overline M]pl=0.1.},
   Doi = {10.1103/physrevlett.99.171802},
   Key = {fds308050}
}

@article{fds308091,
   Author = {Abulencia, and A, and others},
   Title = {Search for new physics in lepton + photon + X events with
             305-pb**(-1) of p anti-p collisions at s**(1/2) = 1.96-
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {97},
   Number = {3},
   Pages = {031801},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.97.031801},
   Abstract = {We present results of a search for anomalous production of
             events containing a charged lepton (either electron or muon)
             and a photon, both with high transverse momentum,
             accompanied by additional signatures, X, including missing
             transverse energy (MET) and additional leptons and photons.
             We use the same kinematic selection criteria as in a
             previous CDF search, but with a substantially larger data
             set, 305 pb-1, a ppbar collision energy of 1.96 TeV, and the
             upgraded CDF II detector. We find 42 Lepton+Photon+MET
             events versus a standard model expectation of 37.3 +- 5.4
             events. The level of excess observed in Run I, 16 events
             with an expectation of 7.6 +- 0.7 events (corresponding to a
             2.7 sigma effect), is not supported by the new data. In the
             signature of Multi-Lepton+Photon+X we observe 31 events
             versus an expectation of 23.0 +- 2.7 events. In this sample
             we find no events with an extra photon or MET and so find no
             events like the one ee+gg+MET event observed in Run
             I.},
   Doi = {10.1103/physrevlett.97.031801},
   Key = {fds308091}
}

@article{fds307754,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for new physics in the dijet mass distribution using
             1 fb -1 of pp collision data at √s=7 TeV
             collected by the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {708},
   Number = {1-2},
   Pages = {37-54},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.01.035},
   Abstract = {Invariant mass distributions of jet pairs (dijets) produced
             in LHC proton-proton collisions at a centre-of-mass energy
             s=7 TeV have been studied using a data set corresponding to
             an integrated luminosity of 1.0 fb -1 recorded in 2011 by
             ATLAS. Dijet masses up to ~4 TeV are observed in the data,
             and no evidence of resonance production over background is
             found. Limits are set at 95% C.L. for several new physics
             hypotheses: excited quarks are excluded for masses below 299
             TeV, axigluons are excluded for masses below 3.32 TeV, and
             colour octet scalar resonances are excluded for masses below
             1.92 TeV. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.01.035},
   Key = {fds307754}
}

@article{fds307972,
   Author = {Aaltonen, T and others},
   Title = {Search for new physics in the mu mu + e/mu + E-slash [sub T]
             channel with a low-p[sub T] lepton threshold at the Collider
             Detector at Fermilab},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {5},
   Pages = {052004},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.052004},
   Abstract = {A search for new physics using three-lepton (trilepton) data
             collected with the CDF II detector and corresponding to an
             integrated luminosity of 976 pb-1 is presented. The standard
             model predicts a low rate of trilepton events, which makes
             some supersymmetric processes, such as chargino-neutralino
             production, measurable in this channel. The μμ+ signature
             is investigated, where ℓ is an electron or a muon, with
             the additional requirement of large missing transverse
             energy. In this analysis, the lepton transverse momenta with
             respect to the beam direction (pT) are as low as 5GeV/c, a
             selection that improves the sensitivity to particles that
             are light as well as to ones that result in leptonically
             decaying tau leptons. At the same time, this low-pT
             selection presents additional challenges due to the
             non-negligible heavy-quark background at low lepton momenta.
             This background is measured with an innovative technique
             using experimental data. Several dimuon and trilepton
             control regions are investigated, and good agreement between
             experimental results and standard-model predictions is
             observed. In the signal region, we observe one three-muon
             event and expect 0.4±0.1μμ+ events from standard-model
             processes. © 2009 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.79.052004},
   Key = {fds307972}
}

@article{fds312131,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Search for new physics in trilepton events and limits on the
             associated chargino-neutralino production at
             CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {1},
   Pages = {012011},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.012011},
   Abstract = {We perform a search for new physics using final states
             consisting of three leptons and a large imbalance in
             transverse momentum resulting from proton-antiproton
             collisions at 1.96 TeV center-of-mass energy. We use data
             corresponding to 5.8fb-1 of integrated luminosity recorded
             by the CDF II detector at the Tevatron collider. Our main
             objective is to investigate possible new low-momentum (down
             to 5GeV/c) multileptonic final states not investigated by
             LHC experiments. Relative to previous CDF analyses, we
             expand the geometric and kinematic coverage of electrons and
             muons and utilize tau leptons that decay hadronically.
             Inclusion of tau leptons is particularly important for
             supersymmetry (SUSY) searches. The results are consistent
             with standard-model predictions within 1.85σ. By optimizing
             our event selection to increase sensitivity to the minimal
             supergravity (mSUGRA) SUSY model, we set limits on the
             associated production of chargino and next-to-lightest
             neutralino, the SUSY partners of the electroweak gauge
             bosons. We exclude cross sections up to 0.1 pb and chargino
             masses up to 168GeV/c2 at 95% C.L., for a suitable set of
             mSUGRA parameters. We also exclude a region of the
             two-dimensional space of the masses of the neutralino and
             the supersymmetric partner of the tau lepton, not previously
             excluded at the Tevatron. © 2014 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.90.012011},
   Key = {fds312131}
}

@article{fds308209,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee,
             S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
             R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
             D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MAC and Cutts,
             D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov,
             VN},
   Title = {Search for new physics in [formula presented] data at DØ
             using SLEUTH: A quasi-model-independent search strategy for
             new physics},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {62},
   Number = {9},
   Pages = {19},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.62.092004},
   Abstract = {We present a quasi-model-independent search for the physics
             responsible for electroweak symmetry breaking. We define
             final states to be studied, and construct a rule that
             identifies a set of relevant variables for any particular
             final state. A new algorithm (“SLEUTH”) searches for
             regions of excess in those variables and quantifies the
             significance of any detected excess. After demonstrating the
             sensitivity of the method, we apply it to the semi-inclusive
             channel (Formula presented) collected in 108 (Formula
             presented) of (Formula presented) collisions at (Formula
             presented) TeV at the DØ experiment during 1992–1996 at
             the Fermilab Tevatron. We find no evidence of new high
             (Formula presented) physics in this sample. © 2000 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.62.092004},
   Key = {fds308209}
}

@article{fds308187,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin,
             B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto,
             J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
             F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MA and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Duperrin, A and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
             VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
             OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher,
             S and Fein, D and Ferbel, T and Filthaut, F and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Fox, H and Frame, KC and Fu,
             S and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin,
             R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grünendahl, S and Gupta,
             A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinmiller, JM and Heinson, AP and Heintz, U and Heuring, T and Hildreth, MD and Hirosky, R and Hobbs, JD and Hoeneisen, B and Huang, Y and Illingworth, R and Ito, AS and Jaffré, M and Jain, S and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahl, W and Kahn, S and Kajfasz, E and Kalinin, AM and Karmanov, D and Karmgard, D and Ke, Z and Kehoe, R and Khanov, A and Kharchilava, A and Kim, SK and Klima, B and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kothari, B and Kotwal,
             AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krivkova, P and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kuznetsov, VE and Landsberg, G and Lee, WM and Leflat, A and Leggett, C and Lehner, F and Li, J and Li, QZ and Li, X and Lima, JG and Lincoln, D and Linn, SL and Linnemann, J and Lipton,
             R and Lucotte, A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AK and Madaras, RJ and Malyshev, VL and Manankov, V and Mao, HS and Marshall,
             T and Martin, MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy, R and McMahon, T and Melanson, HL and Merkin, M and Merritt,
             KW and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mokhov,
             N and Mondal, NK and Montgomery, HE and Moore, RW and Mostafa, M and da
             Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal,
             HA and Negret, JP and Negroni, S and Nunnemann, T and O'Neil, D and Oguri,
             V and Olivier, B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou,
             K and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Pétroff, P and Piegaia, R and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Qian, J and Raja, R and Rajagopalan, S and Ramberg,
             E and Rapidis, PA and Reay, NW and Reucroft, S and Ridel, M and Rijssenbeek, M and Rizatdinova, F and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Sabirov, BM and Sajot,
             G and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov,
             D and Shupe, M and Sidwell, RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery, P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton,
             NR and Steinbrück, G and Stephens, RW and Stichelbaut, F and Stoker, D and Stolin, V and Stone, A and Stoyanova, DA and Strauss, M and Strovink, M and Stutte, L and Sznajder, A and Talby, M and Taylor, W and Tentindo-Repond, S and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and van Gemmeren, P and Vaniev, V and Van Kooten and R and Varelas, N and Vertogradov, LS and Villeneuve-Seguier, F and Volkov,
             AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Womersley, J and Wood, DR and Yamada, R and Yamin, P and Yasuda, T and Yatsunenko, YA and Yip, K and Youssef, S and Yu, J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev, EG and Zylberstejn,
             A},
   Title = {Search for new physics using QUAERO: a general interface to
             D0 event data.},
   Journal = {Physical review letters},
   Volume = {87},
   Number = {23},
   Pages = {231801},
   Year = {2001},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.87.231801},
   Abstract = {We describe QUAERO, a method that (i) enables the automatic
             optimization of searches for physics beyond the standard
             model, and (ii) provides a mechanism for making high energy
             collider data generally available. We apply QUAERO to
             searches for standard model WW, ZZ, and t t macro
             production, to searches for these objects produced through a
             new heavy resonance, and to the first direct search for
             W'-->WZ. Through this interface, we make three data sets
             collected by the D0 experiment at square root of [s] = 1.8
             TeV publicly available.},
   Doi = {10.1103/physrevlett.87.231801},
   Key = {fds308187}
}

@article{fds307897,
   Author = {Aaltonen, and T, and others},
   Title = {Search for New Physics with a Dijet Plus Missing $E_{T}$
             Signature in $pp[over \ifmmode\bar\else\textasciimacron\fi{}]$
             Collisions at $\sqrt{s}=1.96\,\,TeV$},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {13},
   Pages = {131801},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.131801},
   Abstract = {We present results of a signature-based search for new
             physics using a dijet plus missing transverse energy (E(T))
             data sample collected in 2  fb⁻¹ of pp collisions at
             √s=1.96  TeV with the CDF II detector at the Fermilab
             Tevatron. We observe no significant event excess with
             respect to the standard model prediction and extract a 95%
             C.L. upper limit on the cross section times acceptance for a
             potential contribution from a nonstandard model process. The
             search is made by using novel, data-driven techniques for
             estimating backgrounds that are applicable to first searches
             at the LHC.},
   Doi = {10.1103/PhysRevLett.105.131801},
   Key = {fds307897}
}

@article{fds356760,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Search for new resonances decaying to a W or Z boson and a
             Higgs boson in the ℓ+bb¯,
             ℓνbb¯, and νν¯bb¯ channels with pp collisions at
             s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {765},
   Pages = {32-52},
   Year = {2017},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.11.045},
   Abstract = {A search is presented for new resonances decaying to a W or
             Z boson and a Higgs boson in the ℓ+ℓ−bb¯, ℓνbb¯,
             and νν¯bb¯ channels in pp collisions at s=13 TeV with
             the ATLAS detector at the Large Hadron Collider using a
             total integrated luminosity of 3.2 fb−1. The search is
             conducted by looking for a localized excess in the WH/ZH
             invariant or transverse mass distribution. No significant
             excess is observed, and the results are interpreted in terms
             of constraints on a simplified model based on a
             phenomenological Lagrangian of heavy vector
             triplets.},
   Doi = {10.1016/j.physletb.2016.11.045},
   Key = {fds356760}
}

@article{fds321074,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Search for new resonances in events with one lepton and
             missing transverse momentum in pp collisions at √s=13 TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {762},
   Pages = {334-352},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.09.040},
   Abstract = {A search for W′ bosons in events with one lepton (electron
             or muon) and missing transverse momentum is presented. The
             search uses 3.2 fb−1 of pp collision data collected at
             s=13 TeV by the ATLAS experiment at the LHC in 2015. The
             transverse mass distribution is examined and no significant
             excess of events above the level expected from Standard
             Model processes is observed. Upper limits on the W′ boson
             cross-section times branching ratio to leptons are set as a
             function of the W′ mass. Within the Sequential Standard
             Model W′ masses below 4.07 TeV are excluded at the 95%
             confidence level. This extends the limit set using LHC data
             at s=8 TeV by around 800 GeV.},
   Doi = {10.1016/j.physletb.2016.09.040},
   Key = {fds321074}
}

@article{fds349431,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez
             Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {Search for new resonances in mass distributions of jet pairs
             using 139 fb −1 of pp collisions at √s = 13
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {3},
   Year = {2020},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2020)145},
   Abstract = {A search for new resonances decaying into a pair of jets is
             reported using the dataset of proton-proton collisions
             recorded at s = 13 TeV with the ATLAS detector at the Large
             Hadron Collider between 2015 and 2018, corresponding to an
             integrated luminosity of 139 fb−1. The distribution of the
             invariant mass of the two leading jets is examined for local
             excesses above a data-derived estimate of the Standard Model
             background. In addition to an inclusive dijet search, events
             with jets identified as containing b-hadrons are examined
             specifically. No significant excess of events above the
             smoothly falling background spectra is observed. The results
             are used to set cross-section upper limits at 95% confidence
             level on a range of new physics scenarios. Model-independent
             limits on Gaussian-shaped signals are also reported. The
             analysis looking at jets containing b-hadrons benefits from
             improvements in the jet flavour identification at high
             transverse momentum, which increases its sensitivity
             relative to the previous analysis beyond that expected from
             the higher integrated luminosity. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP03(2020)145},
   Key = {fds349431}
}

@article{fds310344,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for new resonances in Wγ and Zγ final states in pp
             collisions at √s=8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {738},
   Pages = {428-447},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.10.002},
   Abstract = {This letter presents a search for new resonances decaying to
             final states with a vector boson produced in association
             with a high transverse momentum photon, Vγ with
             V=W(→ℓν) or Z(→ℓ+ℓ−), where ℓ=e or μ. The
             measurements use 20.3 fb−1 of proton–proton collision
             data at a center–of–mass energy of s=8 TeV recorded with
             the ATLAS detector. No deviations from the Standard Model
             expectations are found, and production cross section limits
             are set at 95% confidence level. Masses of the hypothetical
             aT and ωT states of a benchmark Low Scale Technicolor model
             are excluded in the ranges [275,960] GeV and
             [200,700]∪[750,890] GeV, respectively. Limits at 95%
             confidence level on the production cross section of a
             singlet scalar resonance decaying to Zγ final states have
             also been obtained for masses below 1180
             GeV.},
   Doi = {10.1016/j.physletb.2014.10.002},
   Key = {fds310344}
}

@article{fds356540,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
             Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V},
   Title = {Search for non-resonant Higgs boson pair production in the
             bbℓνℓν final state with the ATLAS detector in pp
             collisions at s=13 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {801},
   Year = {2020},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.135145},
   Abstract = {A search for non-resonant Higgs boson pair production, as
             predicted by the Standard Model, is presented, where one of
             the Higgs bosons decays via the H→bb channel and the other
             via one of the H→WW⁎/ZZ⁎/ττ channels. The analysis
             selection requires events to have at least two b-tagged jets
             and exactly two leptons (electrons or muons) with opposite
             electric charge in the final state. Candidate events
             consistent with Higgs boson pair production are selected
             using a multi-class neural network discriminant. The
             analysis uses 139 fb−1 of pp collision data recorded at a
             centre-of-mass energy of 13 TeV by the ATLAS detector at the
             Large Hadron Collider. An observed (expected) upper limit of
             1.2 (0.9−0.3+0.4) pb is set on the non-resonant Higgs
             boson pair production cross-section at 95% confidence level,
             which is equivalent to 40 (29−9+14) times the value
             predicted in the Standard Model.},
   Doi = {10.1016/j.physletb.2019.135145},
   Key = {fds356540}
}

@article{fds375848,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
             J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
             GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
             Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
             C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
             M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
             SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
   Title = {Search for non-resonant production of semi-visible jets
             using Run 2 data in ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {848},
   Pages = {138324-138324},
   Publisher = {Elsevier BV},
   Year = {2024},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.138324},
   Abstract = {Semi-visible jets, with a significant contribution to the
             event's missing transverse momentum, can arise in strongly
             interacting dark sectors. This results in an event topology
             where one of the jets can be aligned with the direction of
             the missing transverse momentum. The first search for
             semi-visible jets produced via a t-channel mediator exchange
             is presented. The analysis uses proton-proton collisions
             with an integrated luminosity of 139 fb−1 and a
             centre-of-mass energy of 13 TeV, collected with the ATLAS
             detector during the Run 2 of the LHC. No excess over
             Standard Model predictions is observed. Assuming a coupling
             strength of unity between the mediator, a Standard Model
             quark and a dark quark, mediator masses up to 2.7 TeV are
             excluded at the 95% confidence level. Upper limits on the
             coupling strength are also derived.},
   Doi = {10.1016/j.physletb.2023.138324},
   Key = {fds375848}
}

@article{fds310338,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F},
   Title = {Search for nonpointing and delayed photons in the diphoton
             and missing transverse momentum final state in 8 TeV pp
             collisions at the LHC using the ATLAS detector SEARCH for
             NONPOINTING and DELAYED PHOTONS in ⋯ G. AAD et
             al.},
   Journal = {Zeitschrift fur Antikes Christentum},
   Volume = {19},
   Number = {3},
   Pages = {1DUMMY},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.112005},
   Abstract = {© 2014 CERN. © 2014 CERN, for the ATLAS Collaboration.
             Published by the American Physical Society under the terms
             of the »http://creativecommons.org/licenses/by/3.0/»
             Creative Commons Attribution 3.0 License. Further
             distribution of this work must maintain attribution to the
             author(s) and the published article's title, journal
             citation, and DOI.A search has been performed, using the
             full 20.3 fb-1 data sample of 8 TeV proton-proton collisions
             collected in 2012 with the ATLAS detector at the LHC, for
             photons originating from a displaced vertex due to the decay
             of a neutral long-lived particle into a photon and an
             invisible particle. The analysis investigates the diphoton
             plus missing transverse momentum final state, and is
             therefore most sensitive to pair production of long-lived
             particles. The analysis technique exploits the capabilities
             of the ATLAS electromagnetic calorimeter to make precise
             measurements of the flight direction, as well as the time of
             flight, of photons. No excess is observed over the Standard
             Model predictions for background. Exclusion limits are set
             within the context of gauge mediated supersymmetry breaking
             models, with the lightest neutralino being the
             next-to-lightest supersymmetric particle and decaying into a
             photon and gravitino with a lifetime in the range from 250
             ps to about 100 ns.},
   Doi = {10.1103/PhysRevD.90.112005},
   Key = {fds310338}
}

@article{fds307591,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Search for nonpointing photons in the diphoton and ETmiss
             final state in √s=7 TeV proton-proton collisions using the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.012001},
   Abstract = {A search has been performed for photons originating in the
             decay of a neutral long-lived particle, exploiting the
             capabilities of the ATLAS electromagnetic calorimeter to
             make precise measurements of the flight direction of
             photons, as well as the calorimeter's excellent time
             resolution. The search has been made in the diphoton plus
             missing transverse energy final state, using the full data
             sample of 4.8 fb-1 of 7 TeV proton-proton collisions
             collected in 2011 with the ATLAS detector at the LHC. No
             excess is observed above the background expected from
             Standard Model processes. The results are used to set
             exclusion limits in the context of gauge mediated
             supersymmetry breaking models, with the lightest neutralino
             being the next-to-lightest supersymmetric particle and
             decaying with a lifetime in excess of 0.25 ns into a photon
             and a gravitino. © 2013 CERN.},
   Doi = {10.1103/PhysRevD.88.012001},
   Key = {fds307591}
}

@article{fds373909,
   Author = {Amerl, M and Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk
             Cakir, I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori, G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang,
             R and Zhang, J and Berlendis, S and Cheu, E and Cui, Z and Ghosh, A and Johns,
             KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand,
             HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK},
   Title = {Search for nonresonant pair production of Higgs bosons in
             the bb¯bb¯ final state in pp collisions at √s = 13 TeV
             with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {108},
   Number = {5},
   Year = {2023},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.108.052003},
   Abstract = {A search for nonresonant Higgs boson pair production in the
             Formula Presented final state is presented. The analysis
             uses Formula Presented of Formula Presented collision data
             at Formula Presented collected with the ATLAS detector at
             the Large Hadron Collider, and targets both the gluon-gluon
             fusion and vector-boson fusion production modes. No evidence
             of the signal is found and the observed (expected) upper
             limit on the cross section for nonresonant Higgs boson pair
             production is determined to be 5.4 (8.1) times the Standard
             Model predicted cross section at 95% confidence level.
             Constraints are placed on modifiers to the Formula Presented
             and Formula Presented couplings. The observed (expected)
             Formula Presented constraints on the Formula Presented
             coupling modifier, Formula Presented, are determined to be
             Formula Presented (Formula Presented), while the
             corresponding constraints for the Formula Presented coupling
             modifier, Formula Presented, are Formula Presented (Formula
             Presented). In addition, constraints on relevant
             coefficients are derived in the context of the Standard
             Model effective field theory and Higgs effective field
             theory, and upper limits on the Formula Presented production
             cross section are placed in seven Higgs effective field
             theory benchmark scenarios.},
   Doi = {10.1103/PhysRevD.108.052003},
   Key = {fds373909}
}

@article{fds356791,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Alves, GA and Amos, N and Anderson,
             EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov,
             VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland,
             T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {Search for nonstandard higgs bosons using high mass photon
             pairs in p¯p→γγ+2 jets at √s=1.8TeV},
   Journal = {Physical Review Letters},
   Volume = {82},
   Number = {11},
   Pages = {2244-2249},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.82.2244},
   Abstract = {A search has been carried out for events in the channel
             p¯p→γγ+2 Such a signature can characterize the
             production of a nonstandard Higgs boson together with a W or
             Z boson. We refer to this nonstandard Higgs, having standard
             model couplings to vector bosons but no coupling to
             fermions, as a “bosonic Higgs.” With the requirement of
             two high transverse energy photons and two jets, the
             diphoton mass (mγγ) distribution is consistent with
             expected background. A 90 (95)% confidence level (C.L.)
             upper limit on the cross section as a function of mass is
             calculated, ranging from 0.60 (0.80) pb for mγγ =65GeV/c2
             to 0.26 (0.34) pb for mγγ=150GeV/c2, corresponding to a
             95% C.L. lower limit on the mass of a bosonic Higgs of
             78.5GeV/c2. © 1999 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.82.2244},
   Key = {fds356791}
}

@article{fds310345,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for pair and single production of new heavy quarks
             that decay to a Z boson and a third-generation quark in pp
             collisions at √ S = 8TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2014)104},
   Abstract = {Abstract: A search is presented for the production of new
             heavy quarks that decay to a Z boson and a third-generation
             Standard Model quark. In the case of a new charge +2/3 quark
             (T ), the decay targeted is T → Zt, while the decay
             targeted for a new charge −1/3 quark (B) is B → Zb. The
             search is performed with a dataset corresponding to 20.3
             fb−1 of pp collisions at (Formula presented.) TeV recorded
             in 2012 with the ATLAS detector at the CERN Large Hadron
             Collider. Selected events contain a high transverse momentum
             Z boson candidate reconstructed from a pair of oppositely
             charged same-flavor leptons (electrons or muons), and are
             analyzed in two channels defined by the absence or presence
             of a third lepton. Hadronic jets, in particular those with
             properties consistent with the decay of a b-hadron, are also
             required to be present in selected events. Different
             requirements are made on the jet activity in the event in
             order to enhance the sensitivity to either heavy quark pair
             production mediated by the strong interaction, or single
             production mediated by the electroweak interaction. No
             significant excess of events above the Standard Model
             expectation is observed, and lower limits are derived on the
             mass of vector-like T and B quarks under various branching
             ratio hypotheses, as well as upper limits on the magnitude
             of electroweak coupling parameters.},
   Doi = {10.1007/JHEP11(2014)104},
   Key = {fds310345}
}

@article{fds356636,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Search for pair and single production of vectorlike quarks
             in final states with at least one Z boson decaying into a
             pair of electrons or muons in pp collision data collected
             with the ATLAS detector at s =13 TeV},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {11},
   Year = {2018},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.112010},
   Abstract = {A search for vectorlike quarks is presented, which targets
             their decay into a Z boson and a third-generation Standard
             Model quark. In the case of a vectorlike quark T (B) with
             charge +2/3e (-1/3e), the decay searched for is T→Zt
             (B→Zb). Data for this analysis were taken during 2015 and
             2016 with the ATLAS detector at the Large Hadron Collider
             and correspond to an integrated luminosity of 36.1 fb-1 of
             pp collisions at s=13 TeV. The final state used is
             characterized by the presence of b-tagged jets, as well as a
             Z boson with high transverse momentum, which is
             reconstructed from a pair of opposite-sign same-flavor
             leptons. Pair and single production of vectorlike quarks are
             both taken into account and are each searched for using
             optimized dileptonic exclusive and trileptonic inclusive
             event selections. In these selections, the high scalar sum
             of jet transverse momenta, the presence of
             high-transverse-momentum large-radius jets, as well as - in
             the case of the single-production selections - the presence
             of forward jets are used. No significant excess over the
             background-only hypothesis is found and exclusion limits at
             95% confidence level allow masses of vectorlike quarks of
             mT>1030 GeV (mT>1210 GeV) and mB>1010 GeV (mB>1140 GeV) in
             the singlet (doublet) model. In the case of 100% branching
             ratio for T→Zt (B→Zb), the limits are mT>1340 GeV
             (mB>1220 GeV). Limits at 95% confidence level are also set
             on the coupling to Standard Model quarks for given
             vectorlike quark masses.},
   Doi = {10.1103/PhysRevD.98.112010},
   Key = {fds356636}
}

@article{fds307697,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Search for pair production of a heavy up-type quark decaying
             to a W boson and a b quark in the lepton + jets channel with
             the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {26},
   Pages = {261802},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.108.261802},
   Abstract = {A search is presented for production of a heavy up-type
             quark (t') together with its antiparticle, assuming
             subsequent decay to a W boson and a b quark, t't[over
             ¯]'→W(+)bW(-)b[over ¯]. The search is based on 1.04
             fb(-1) of proton-proton collisions at √[s]=7 TeV collected
             by the ATLAS detector at the CERN Large Hadron Collider.
             Data are analyzed in the lepton+jets final state,
             characterized by a high transverse momentum isolated
             electron or muon, high missing transverse momentum, and at
             least three jets. No significant excess of events above the
             background expectation is observed. A 95% C.L. lower limit
             of 404 GeV is set for the mass of the t'
             quark.},
   Doi = {10.1103/physrevlett.108.261802},
   Key = {fds307697}
}

@article{fds307690,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
             PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas,
             CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
             X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC},
   Title = {Search for pair production of a new b' quark that decays
             into a Z boson and a bottom quark with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {7},
   Pages = {071801},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.109.071801},
   Abstract = {A search is reported for the pair production of a new quark
             b' with at least one b' decaying to a Z boson and a bottom
             quark. The data, corresponding to 2.0 fb(-1) of integrated
             luminosity, were collected from pp collisions at √s = 7
             TeV with the ATLAS detector at the CERN Large Hadron
             Collider. Using events with a b-tagged jet and a Z boson
             reconstructed from opposite-charge electrons, the mass
             distribution of large transverse momentum b' candidates is
             tested for an enhancement. No evidence for a b' signal is
             detected in the observed mass distribution, resulting in the
             exclusion at a 95% confidence level of b' quarks with masses
             m (b') < 400 GeV that decay entirely via b' → Z+b. In the
             case of a vectorlike singlet b' mixing solely with the third
             standard model generation, masses m(b') < 358 GeV are
             excluded.},
   Doi = {10.1103/physrevlett.109.071801},
   Key = {fds307690}
}

@article{fds313613,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Search for pair production of a new heavy quark that decays
             into a W boson and a light quark in pp collisions at s =8
             TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {December},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.112007},
   Abstract = {A search is presented for pair production of a new heavy
             quark (Q) that decays into a W boson and a light quark (q)
             in the final state where one W boson decays leptonically (to
             an electron or muon plus a neutrino) and the other W boson
             decays hadronically. The analysis is performed using an
             integrated luminosity of 20.3 fb-1 of pp collisions at s=8
             TeV collected by the ATLAS detector at the LHC. No evidence
             of QQ¯ production is observed. New chiral quarks with
             masses below 690 GeV are excluded at 95% confidence level,
             assuming BR(Q→Wq)=1. Results are also interpreted in the
             context of vectorlike quark models, resulting in the limits
             on the mass of a vectorlike quark in the two-dimensional
             plane of BR(Q→Wq) versus BR(Q→Hq).},
   Doi = {10.1103/PhysRevD.92.112007},
   Key = {fds313613}
}

@article{fds307855,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Ákesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S},
   Title = {Search for pair production of first or second generation
             leptoquarks in proton-proton collisions at √s=7TeV using
             the ATLAS detector at the LHC},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {83},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.112006},
   Abstract = {This paper describes searches for the pair production of
             first or second generation scalar leptoquarks using 35pb-1
             of proton-proton collision data recorded by the ATLAS
             detector at √s=7TeV. Leptoquarks are searched in events
             with two oppositely-charged muons or electrons and at least
             two jets, and in events with one muon or electron, missing
             transverse momentum and at least two jets. After event
             selection, the observed yields are consistent with the
             predicted backgrounds. Leptoquark production is excluded at
             the 95 CL for masses MLQ<376 (319) GeV and MLQ<422 (362) GeV
             for first and second generation scalar leptoquarks,
             respectively, when assuming the branching fraction of a
             leptoquark to a charged lepton is equal to 1.0 (0.5). ©
             2011 American Physical Society.},
   Doi = {10.1103/PhysRevD.83.112006},
   Key = {fds307855}
}

@article{fds321111,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov,
             A},
   Title = {Search for pair production of gluinos decaying via stop and
             sbottom in events with b -jets and large missing transverse
             momentum in pp collisions at s =13 TeV with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.032003},
   Abstract = {A search for supersymmetry involving the pair production of
             gluinos decaying via third-generation squarks to the
             lightest neutralino (χ10) is reported. It uses an LHC
             proton-proton data set at a center-of-mass energy s=13 TeV
             with an integrated luminosity of 3.2 fb-1 collected with the
             ATLAS detector in 2015. The signal is searched for in events
             containing several energetic jets, of which at least three
             must be identified as b jets, large missing transverse
             momentum, and, potentially, isolated electrons or muons.
             Large-radius jets with a high mass are also used to identify
             highly boosted top quarks. No excess is found above the
             predicted background. For χ10 masses below approximately
             700 GeV, gluino masses of less than 1.78 TeV and 1.76 TeV
             are excluded at the 95% C.L. in simplified models of the
             pair production of gluinos decaying via sbottom and stop,
             respectively. These results significantly extend the
             exclusion limits obtained with the s=8 TeV data
             set.},
   Doi = {10.1103/PhysRevD.94.032003},
   Key = {fds321111}
}

@article{fds307632,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
             Costa, JJBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Bege, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
             JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, R and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Busey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, JJ and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas,
             CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, JJ and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A},
   Title = {Search for pair production of heavy top-like quarks decaying
             to a high-pT W boson and a b
             quark in the lepton plus jets final state at √s=7
             TeV with the ATLAS detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {718},
   Number = {4-5},
   Pages = {1284-1302},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.11.071},
   Abstract = {© 2012 CERN A search is presented for production of a heavy
             up-type quark (t′) together with its antiparticle,
             assuming a significant branching ratio for subsequent decay
             into a W boson and a b quark. The search is based on 4.7
             fb−1 of pp collisions at s=7 TeV recorded in 2011 with the
             ATLAS detector at the CERN Large Hadron Collider. Data are
             analyzed in the lepton + jets final state, characterized by
             a high-transverse-momentum isolated electron or muon, large
             missing transverse momentum and at least three jets. The
             analysis strategy relies on the substantial boost of the W
             bosons in the t′t¯′ signal when mt′≳400 GeV. No
             significant excess of events above the Standard Model
             expectation is observed and the result of the search is
             interpreted in the context of fourth-generation and
             vector-like quark models. Under the assumption of a
             branching ratio BR(t′→Wb)=1, a fourth-generation t′
             quark with mass lower than 656 GeV is excluded at 95%
             confidence level. In addition, in light of the recent
             discovery of a new boson of mass ∼126 GeV at the LHC,
             upper limits are derived in the two-dimensional plane of
             BR(t′→Wb) versus BR(t′→Ht), where H is the Standard
             Model Higgs boson, for vector-like quarks of various
             masses.},
   Doi = {10.1016/j.physletb.2012.11.071},
   Key = {fds307632}
}

@article{fds356667,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
   Title = {Search for pair production of heavy vector-like quarks
             decaying into high-p T W bosons and top quarks in
             the lepton-plus-jets final state in pp collisions at √s=13
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {8},
   Year = {2018},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2018)048},
   Abstract = {A search is presented for the pair production of heavy
             vector-like B quarks, primarily targeting B quark decays
             into a W boson and a top quark. The search is based on 36.1
             fb−1 of pp collisions at s=13 TeV recorded in 2015 and
             2016 with the ATLAS detector at the CERN Large Hadron
             Collider. Data are analysed in the lepton-plus-jets final
             state, characterised by a high-transverse-momentum isolated
             electron or muon, large missing transverse momentum, and
             multiple jets, of which at least one is b-tagged. No
             significant deviation from the Standard Model expectation is
             observed. The 95% confidence level lower limit on the B mass
             is 1350 GeV assuming a 100% branching ratio to Wt. In the
             SU(2) singlet scenario, the lower mass limit is 1170 GeV.
             The 100% branching ratio limits are found to be also
             applicable to heavy vector-like X production, with charge
             +5/3, that decay into Wt. This search is also sensitive to a
             heavy vector-like B quark decaying into other final states
             (Zb and Hb) and thus mass limits on B production are set as
             a function of the decay branching ratios.[Figure not
             available: see fulltext.].},
   Doi = {10.1007/JHEP08(2018)048},
   Key = {fds356667}
}

@article{fds356733,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Search for pair production of heavy vector-like quarks
             decaying to high-p T W bosons and b quarks in the
             lepton-plus-jets final state in pp collisions at √s=13 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {10},
   Year = {2017},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2017)141},
   Abstract = {A search is presented for the pair production of heavy
             vector-like T quarks, primarily targeting the T quark decays
             to a W boson and a b-quark. The search is based on 36.1
             fb−1 of pp collisions at s=13 TeV recorded in 2015 and
             2016 with the ATLAS detector at the CERN Large Hadron
             Collider. Data are analysed in the lepton-plus-jets final
             state, including at least one b-tagged jet and a
             large-radius jet identified as originating from the hadronic
             decay of a high-momentum W boson. No significant deviation
             from the Standard Model expectation is observed in the
             reconstructed T mass distribution. The observed 95%
             confidence level lower limit on the T mass are 1350 GeV
             assuming 100% branching ratio to Wb. In the SU(2) singlet
             scenario, the lower mass limit is 1170 GeV. This search is
             also sensitive to a heavy vector-like B quark decaying to Wt
             and other final states. The results are thus reinterpreted
             to provide a 95% confidence level lower limit on the B quark
             mass at 1250 GeV assuming 100% branching ratio to Wt; in the
             SU(2) singlet scenario, the limit is 1080 GeV. Mass limits
             on both T and B production are also set as a function of the
             decay branching ratios. The 100% branching ratio limits are
             found to be applicable to heavy vector-like Y and X
             production that decay to Wb and Wt, respectively.},
   Doi = {10.1007/JHEP10(2017)141},
   Key = {fds356733}
}

@article{fds356641,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
   Title = {Search for pair production of heavy vectorlike quarks
             decaying into hadronic final states in pp collisions at s
             =13 TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {9},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.092005},
   Abstract = {A search is presented for the pair production of heavy
             vectorlike quarks, TT or BB, that decay into final states
             with jets and no reconstructed leptons. Jets in the final
             state are classified using a deep neural network as arising
             from hadronically decaying W/Z bosons, Higgs bosons, top
             quarks, or background. The analysis uses data from the ATLAS
             experiment corresponding to 36.1 fb-1 of proton-proton
             collisions with a center-of-mass energy of s=13 TeV
             delivered by the Large Hadron Collider in 2015 and 2016. No
             significant deviation from the Standard Model expectation is
             observed. Results are interpreted assuming the vectorlike
             quarks decay into a Standard Model boson and a
             third-generation-quark, T→Wb,Ht,Zt or B→Wt,Hb,Zb, for a
             variety of branching ratios. At 95% confidence level, the
             observed (expected) lower limit on the vectorlike B-quark
             mass for a weak-isospin doublet (B, Y) is 950 (890) GeV, and
             the lower limits on the masses for the pure decays B→Hb
             and T→Ht, where these results are strongest, are 1010
             (970) GeV and 1010 (1010) GeV, respectively.},
   Doi = {10.1103/PhysRevD.98.092005},
   Key = {fds356641}
}

@article{fds321100,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for pair production of Higgs bosons in the bbbb final
             state using proton-proton collisions at √s =13 TeV with
             the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.052002},
   Abstract = {A search for Higgs-boson pair production in the bbbb final
             state is carried out with 3.2 fb-1 of proton-proton
             collision data collected at s=13 TeV with the ATLAS
             detector. The data are consistent with the estimated
             background and are used to set upper limits on the
             production cross section of Higgs-boson pairs times
             branching ratio to bbbb for both nonresonant and resonant
             production. In the case of resonant production of
             Kaluza-Klein gravitons within the Randall-Sundrum model,
             upper limits in the 24 to 91 fb range are obtained for
             masses between 600 and 3000 GeV, at the 95% confidence
             level. The production cross section times branching ratio
             for nonresonant Higgs-boson pairs is also constrained to be
             less than 1.22 pb, at the 95% confidence
             level.},
   Doi = {10.1103/PhysRevD.94.052002},
   Key = {fds321100}
}

@article{fds347449,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for pair production of Higgs bosons in the bb¯ bb¯
             final state using proton-proton collisions at √s=13 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {1},
   Year = {2019},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2019)030},
   Abstract = {A search for Higgs boson pair production in the bb¯ bb¯
             final state is carried out with up to 36.1 fb−1 of LHC
             proton-proton collision data collected at s=13 TeV with the
             ATLAS detector in 2015 and 2016. Three benchmark signals are
             studied: a spin-2 graviton decaying into a Higgs boson pair,
             a scalar resonance decaying into a Higgs boson pair, and
             Standard Model non-resonant Higgs boson pair production. Two
             analyses are carried out, each implementing a particular
             technique for the event reconstruction that targets Higgs
             bosons reconstructed as pairs of jets or single boosted
             jets. The resonance mass range covered is 260–3000 GeV.
             The analyses are statistically combined and upper limits on
             the production cross section of Higgs boson pairs times
             branching ratio to bb¯ bb¯ are set in each model. No
             significant excess is observed; the largest deviation of
             data over prediction is found at a mass of 280 GeV,
             corresponding to 2.3 standard deviations globally. The
             observed 95% confidence level upper limit on the
             non-resonant production is 13 times the Standard Model
             prediction.[Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP01(2019)030},
   Key = {fds347449}
}

@article{fds356642,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for pair production of Higgsinos in final states with
             at least three b -tagged jets in s =13 TeV pp collisions
             using the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {9},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.092002},
   Abstract = {A search for pair production of the supersymmetric partners
             of the Higgs boson (higgsinos H) in gauge-mediated scenarios
             is reported. Each higgsino is assumed to decay to a Higgs
             boson and a gravitino. Two complementary analyses, targeting
             high- and low-mass signals, are performed to maximize
             sensitivity. The two analyses utilize LHC pp collision data
             at a center-of-mass energy s=13 TeV, the former with an
             integrated luminosity of 36.1 fb-1 and the latter with 24.3
             fb-1, collected with the ATLAS detector in 2015 and 2016.
             The search is performed in events containing missing
             transverse momentum and several energetic jets, at least
             three of which must be identified as b-quark jets. No
             significant excess is found above the predicted background.
             Limits on the cross section are set as a function of the
             mass of the H in simplified models assuming production via
             mass-degenerate higgsinos decaying to a Higgs boson and a
             gravitino. Higgsinos with masses between 130 and 230 GeV and
             between 290 and 880 GeV are excluded at the 95% confidence
             level. Interpretations of the limits in terms of the
             branching ratio of the higgsino to a Z boson or a Higgs
             boson are also presented, and a 45% branching ratio to a
             Higgs boson is excluded for mH≈400 GeV.},
   Doi = {10.1103/PhysRevD.98.092002},
   Key = {fds356642}
}

@article{fds307663,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for pair production of massive particles decaying
             into three quarks with the ATLAS detector in √s = 7 TeV pp
             collisions at the LHC},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {12},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP12(2012)086},
   Abstract = {A search is conducted for hadronic three-body decays of a
             new massive coloured particle in √s = 7 TeV pp collisions
             at the LHC using an integrated luminosity of 4.6 fb-1
             collected by the ATLAS detector. Supersymmetric gluino pair
             production in the context of a model with R-parity violation
             is used as a benchmark scenario. The analysis is divided
             into two search channels, each optimised separately for
             their sensitivity to high-mass and low-mass gluino
             production. The first search channel uses a stringent
             selection on the transverse momentum of the six leading jets
             and is performed as a counting experiment. The second search
             channel focuses on low-mass gluinos produced with a large
             boost. Large-radius jets are selected and the invariant mass
             of each of the two leading jets is used as a discriminant
             between the signal and the background. The results are found
             to be consistent with Standard Model expectations and limits
             are set on the allowed gluino mass.[Figure not available:
             see fulltext.] © 2012 Cern for the benefit of the ATLAS
             collaboration.},
   Doi = {10.1007/JHEP12(2012)086},
   Key = {fds307663}
}

@article{fds355954,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
             M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
   Title = {Search for pair production of scalar leptoquarks decaying
             into first- or second-generation leptons and top quarks in
             proton–proton collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {4},
   Year = {2021},
   Month = {April},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09009-8},
   Abstract = {A search for pair production of scalar leptoquarks, each
             decaying into either an electron or a muon and a top quark,
             is presented. This is the first leptoquark search using
             ATLAS data to investigate top-philic cross-generational
             couplings that could provide explanations for recently
             observed anomalies in B meson decays. This analysis targets
             high leptoquark masses which cause the decay products of
             each resultant top quark to be contained within a single
             high-pT large-radius jet. The full Run 2 dataset is
             exploited, consisting of 139fb-1 of data collected from
             proton–proton collisions at s=13TeV from 2015 to 2018 with
             the ATLAS detector at the CERN Large Hadron Collider. In the
             absence of any significant deviation from the background
             expectation, lower limits on the leptoquark masses are set
             at 1480GeV and 1470GeV for the electron and muon channel,
             respectively.},
   Doi = {10.1140/epjc/s10052-021-09009-8},
   Key = {fds355954}
}

@article{fds307593,
   Author = {Aaltonen, T and Albin, E and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
             A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
             B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
             A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
             F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and d'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
             P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu,
             C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes,
             L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
             C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
             K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
             J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
             P and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson,
             JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Search for pair production of strongly interacting particles
             decaying to pairs of jets in pp collisions at √s=1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {3},
   Pages = {031802},
   Year = {2013},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.111.031802},
   Abstract = {We present a search for the pair production of a narrow
             nonstandard-model strongly interacting particle that decays
             to a pair of quarks or gluons, leading to a final state with
             four hadronic jets. We consider both nonresonant production
             via an intermediate gluon as well as resonant production via
             a distinct nonstandard-model intermediate strongly
             interacting particle. We use data collected by the CDF
             experiment in proton-antiproton collisions at √[s]=1.96
             TeV corresponding to an integrated luminosity of 6.6 fb(-1).
             We find the data to be consistent with nonresonant
             production. We report limits on σ(pp[over ¯]→jjjj) as a
             function of the masses of the hypothetical intermediate
             particles. Upper limits on the production cross sections for
             nonstandard-model particles in several resonant and
             nonresonant processes are also derived.},
   Doi = {10.1103/physrevlett.111.031802},
   Key = {fds307593}
}

@article{fds307902,
   Author = {Aaltonen, and T, and others},
   Title = {Search for Pair Production of Supersymmetric Top Quarks in
             Dilepton Events from $p\bar{p}$ Collisions at $\sqrt{s}$ =
             1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {25},
   Pages = {251801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.251801},
   Abstract = {http://arxiv.org/abs/0912.1308},
   Doi = {10.1103/PhysRevLett.104.251801},
   Key = {fds307902}
}

@article{fds375364,
   Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
             BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
             P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez, AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
             KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E},
   Title = {Search for pair production of third-generation leptoquarks
             decaying into a bottom quark and a τ -lepton with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {11},
   Year = {2023},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-12104-7},
   Abstract = {A search for pair-produced scalar or vector leptoquarks
             decaying into a b-quark and a τ -lepton is presented using
             the full LHC Run 2 (2015–2018) data sample of 139 fb - 1
             collected with the ATLAS detector in proton–proton
             collisions at a centre-of-mass energy of s=13 TeV. Events in
             which at least one τ -lepton decays hadronically are
             considered, and multivariate discriminants are used to
             extract the signals. No significant deviations from the
             Standard Model expectation are observed and 95%
             confidence-level upper limits on the production
             cross-section are derived as a function of leptoquark mass
             and branching ratio B into a τ -lepton and b-quark. For
             scalar leptoquarks, masses below 1460 GeV are excluded
             assuming B= 100 %, while for vector leptoquarks the
             corresponding limit is 1650 GeV (1910 GeV) in the
             minimal-coupling (Yang–Mills) scenario.},
   Doi = {10.1140/epjc/s10052-023-12104-7},
   Key = {fds375364}
}

@article{fds357657,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
             J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler,
             A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and An, F and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
             Bella, L and Aranzabal, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arguin, JF and Argyropoulos,
             S},
   Title = {Search for pair production of third-generation scalar
             leptoquarks decaying into a top quark and a τ-lepton in pp
             collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {6},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2021)179},
   Abstract = {A search for pair production of third-generation scalar
             leptoquarks decaying into a top quark and a τ-lepton is
             presented. The search is based on a dataset of pp collisions
             at s = 13 TeV recorded with the ATLAS detector during Run 2
             of the Large Hadron Collider, corresponding to an integrated
             luminosity of 139 fb−1. Events are selected if they have
             one light lepton (electron or muon) and at least one
             hadronically decaying τ -lepton, or at least two light
             leptons. In addition, two or more jets, at least one of
             which must be identified as containing b-hadrons, are
             required. Six final states, defined by the multiplicity and
             flavour of lepton candidates, are considered in the
             analysis. Each of them is split into multiple event
             categories to simultaneously search for the signal and
             constrain several leading backgrounds. The signal-rich event
             categories require at least one hadronically decaying
             τ-lepton candidate and exploit the presence of energetic
             final-state objects, which is characteristic of signal
             events. No significant excess above the Standard Model
             expectation is observed in any of the considered event
             categories, and 95% CL upper limits are set on the
             production cross section as a function of the leptoquark
             mass, for different assumptions about the branching
             fractions into tτ and bν. Scalar leptoquarks decaying
             exclusively into tτ are excluded up to masses of 1.43 TeV
             while, for a branching fraction of 50% into tτ, the lower
             mass limit is 1.22 TeV. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP06(2021)179},
   Key = {fds357657}
}

@article{fds336451,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Arnaez, O and Arnold, H and Arratia, M},
   Title = {Search for pair production of up-type vector-like quarks and
             for four-top-quark events in final states with multiple
             b-jets with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {7},
   Publisher = {Springer Nature},
   Year = {2018},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2018)089},
   Abstract = {A search for pair production of up-type vector-like quarks
             (T) with a significant branching ratio into a top quark and
             either a Standard Model Higgs boson or a Z boson is
             presented. The same analysis is also used to search for
             four-top-quark production in several new physics scenarios.
             The search is based on a dataset of pp collisions at s=13
             TeV recorded in 2015 and 2016 with the ATLAS detector at the
             CERN Large Hadron Collider and corresponds to an integrated
             luminosity of 36.1 fb-1. Data are analysed in the
             lepton+jets final state, characterised by an isolated
             electron or muon with high transverse momentum, large
             missing transverse momentum and multiple jets, as well as
             the jets + ETmiss final state, characterised by multiple
             jets and large missing transverse momentum. The search
             exploits the high multiplicity of jets identified as
             originating from b-quarks, and the presence of boosted,
             hadronically decaying top quarks and Higgs bosons
             reconstructed as large-radius jets, characteristic of signal
             events. No significant excess above the Standard Model
             expectation is observed, and 95% CL upper limits are set on
             the production cross sections for the different signal
             processes considered. These cross-section limits are used to
             derive lower limits on the mass of a vector-like T quark
             under several branching ratio hypotheses assuming
             contributions from T ? W b, Zt, Ht decays. The 95% CL
             observed lower limits on the T quark mass range between 0.99
             TeV and 1.43 TeV for all possible values of the branching
             ratios into the three decay modes considered, significantly
             extending the reach beyond that of previous searches.
             Additionally, upper limits on anomalous four-top-quark
             production are set in the context of an effective field
             theory model, as well as in an universal extra dimensions
             model.[Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP07(2018)089},
   Key = {fds336451}
}

@article{fds356745,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Verzini, MJA and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Santos,
             SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Search for pair production of vector-like top quarks in
             events with one lepton, jets, and missing transverse
             momentum in √s=13 TeV pp collisions with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {8},
   Year = {2017},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2017)052},
   Abstract = {The results of a search for vector-like top quarks using
             events with exactly one lepton, at least four jets, and
             large missing transverse momentum are reported. The search
             is optimised for pair production of vector-like top quarks
             in the Z() t + X decay channel. LHC pp collision data at a
             centre-of-mass energy of s=13 TeV recorded by the ATLAS
             detector in 2015 and 2016 are used, corresponding to an
             integrated luminosity of 36.1 fb−1. No significant excess
             over the Standard Model expectation is seen and upper limits
             on the production cross-section of a vector-like T quark
             pair as a function of the T quark mass are derived. The
             observed (expected) 95% CL lower limits on the T mass are
             870 GeV (890 GeV) for the weak-isospin singlet model, 1.05
             TeV (1.06 TeV) for the weak-isospin doublet model and 1.16
             TeV (1.17 TeV) for the pure Zt decay mode. Limits are also
             set on the mass as a function of the decay branching ratios,
             excluding large parts of the parameter space for masses
             below 1 TeV.[Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP08(2017)052},
   Key = {fds356745}
}

@article{fds307739,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for pair-produced heavy quarks decaying to Wq in the
             two-lepton channel at √(s)=7TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.012007},
   Abstract = {A search is presented for heavy-quark pair production (QQ̄)
             under the decay hypothesis QQ̄→W+qW-q̄ with q=d, s, b
             for up-type Q or q=u, c for down-type Q. The search is
             performed with 1.04fb-1 of integrated luminosity from pp
             collisions at √s=7TeV collected by the ATLAS detector at
             the CERN LHC. Dilepton final states are selected, requiring
             large missing transverse momentum and at least two jets.
             Mass reconstruction of heavy-quark candidates is performed
             by assuming that the W boson decay products are nearly
             collinear. The data are in agreement with standard model
             expectations; a heavy quark with mass less than 350 GeV is
             excluded at 95% confidence level. © 2012 CERN. Published by
             the American Physical Society under the terms of the
             http://creativecommons.org/licenses/by/ 3.0/ Creative
             Commons Attribution 3.0 License. Further distribution of
             this work must maintain attribution to the author(s) and the
             published article's title, journal citation, and
             DOI.},
   Doi = {10.1103/PhysRevD.86.012007},
   Key = {fds307739}
}

@article{fds325305,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for pair-produced long-lived neutral particles
             decaying to jets in the ATLAS hadronic calorimeter in pp
             collisions at s=8TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {743},
   Pages = {15-34},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.02.015},
   Abstract = {The ATLAS detector at the Large Hadron Collider at CERN is
             used to search for the decay of a scalar boson to a pair of
             long-lived particles, neutral under the Standard Model gauge
             group, in 20.3fb-1 of data collected in proton-proton
             collisions at s=8TeV. This search is sensitive to long-lived
             particles that decay to Standard Model particles producing
             jets at the outer edge of the ATLAS electromagnetic
             calorimeter or inside the hadronic calorimeter. No
             significant excess of events is observed. Limits are
             reported on the product of the scalar boson production cross
             section times branching ratio into long-lived neutral
             particles as a function of the proper lifetime of the
             particles. Limits are reported for boson masses from 100 GeV
             to 900 GeV, and a long-lived neutral particle mass from 10
             GeV to 150 GeV.},
   Doi = {10.1016/j.physletb.2015.02.015},
   Key = {fds325305}
}

@article{fds307649,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim,
             A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E},
   Title = {Search for pair-produced massive coloured scalars in
             four-jet final states with the ATLAS detector in
             proton–proton collisions at √s =7 TeV},
   Journal = {European Physical Journal C},
   Volume = {73},
   Number = {1},
   Pages = {1-20},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2263-z},
   Abstract = {A search for pair-produced massive coloured scalar particles
             decaying to a four-jet final state is performed by the ATLAS
             experiment at the LHC in proton–proton collisions at √s
             = 7 TeV. The analysed data sample corresponds to an
             integrated luminosity of 4.6 fb<sup>−1</sup>. No deviation
             from the Standard Model is observed in the invariant mass
             spectrum of the two-jet pairs. A limit on the scalar gluon
             pair production cross section of 70 pb (10 pb) is obtained
             at the 95 % confidence level for a scalar gluon mass of 150
             GeV (350 GeV). Interpreting these results as mass limits on
             scalar gluons, masses ranging from 150 GeV to 287 GeV are
             excluded at the 95 % confidence level.},
   Doi = {10.1140/epjc/s10052-012-2263-z},
   Key = {fds307649}
}

@article{fds310364,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for pair-produced third-generation squarks decaying
             via charm quarks or in compressed supersymmetric scenarios
             in pp collisions at √s =8TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.052008},
   Abstract = {Results of a search for supersymmetry via direct production
             of third-generation squarks are reported, using 20.3fb-1 of
             proton-proton collision data at s=8TeV recorded by the ATLAS
             experiment at the LHC in 2012. Two different analysis
             strategies based on monojetlike and c-tagged event
             selections are carried out to optimize the sensitivity for
             direct top squark-pair production in the decay channel to a
             charm quark and the lightest neutralino (t∼1→c+χ∼10)
             across the top squark-neutralino mass parameter space. No
             excess above the Standard Model background expectation is
             observed. The results are interpreted in the context of
             direct pair production of top squarks and presented in terms
             of exclusion limits in the (mt∼1, mχ∼10) parameter
             space. A top squark of mass up to about 240 GeV is excluded
             at 95% confidence level for arbitrary neutralino masses,
             within the kinematic boundaries. Top squark masses up to 270
             GeV are excluded for a neutralino mass of 200 GeV. In a
             scenario where the top squark and the lightest neutralino
             are nearly degenerate in mass, top squark masses up to 260
             GeV are excluded. The results from the monojetlike analysis
             are also interpreted in terms of compressed scenarios for
             top squark-pair production in the decay channel
             t∼1→b+ff′+χ∼10 and sbottom pair production with
             b∼1→b+χ∼10, leading to a similar exclusion for nearly
             mass-degenerate third-generation squarks and the lightest
             neutralino. The results in this paper significantly extend
             previous results at colliders.},
   Doi = {10.1103/PhysRevD.90.052008},
   Key = {fds310364}
}

@article{fds374026,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
             A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
             W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
             PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
             Ferraz, V and Arcangeletti, C and Arce, ATH and Arena,
             E},
   Title = {Search for pair-produced vector-like top and bottom partners
             in events with large missing transverse momentum in pp
             collisions with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {8},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11790-7},
   Abstract = {A search for pair-produced vector-like quarks using events
             with exactly one lepton (e or μ), at least four jets
             including at least one b-tagged jet, and large missing
             transverse momentum is presented. Data from proton–proton
             collisions at a centre-of-mass energy of s= 13 TeV ,
             recorded by the ATLAS detector at the LHC from 2015 to 2018
             and corresponding to an integrated luminosity of 139 fb - 1
             , are analysed. Vector-like partners T and B of the top and
             bottom quarks are considered, as is a vector-like X with
             charge + 5 / 3 , assuming their decay into a W, Z, or Higgs
             boson and a third-generation quark. No significant
             deviations from the Standard Model expectation are observed.
             Upper limits on the production cross-section of T and B
             quark pairs as a function of their mass are derived for
             various decay branching ratio scenarios. The strongest lower
             limits on the masses are 1.59 TeV assuming mass-degenerate
             vector-like quarks and branching ratios corresponding to the
             weak-isospin doublet model, and 1.47 TeV (1.46 TeV) for
             exclusive T→ Zt (B/ X→ Wt) decays. In addition, lower
             limits on the T and B quark masses are derived for all
             possible branching ratios.},
   Doi = {10.1140/epjc/s10052-023-11790-7},
   Key = {fds374026}
}

@article{fds372125,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
             SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Aly, M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
             CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
   Title = {Search for pair-production of vector-like quarks in pp
             collision events at s=13 TeV with at least one leptonically
             decaying Z boson and a third-generation quark with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {843},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.138019},
   Abstract = {A search for the pair-production of vector-like quarks
             optimized for decays into a Z boson and a third-generation
             Standard Model quark is presented, using the full Run 2
             dataset corresponding to 139fb−1 of pp collisions at
             s=13TeV, collected in 2015–2018 with the ATLAS detector at
             the Large Hadron Collider. The targeted final state is
             characterized by the presence of a Z boson with high
             transverse momentum, reconstructed from a pair of
             same-flavour leptons with opposite-sign charges, as well as
             by the presence of b-tagged jets and high-transverse-momentum
             large-radius jets reconstructed from calibrated
             smaller-radius jets. Events with exactly two or at least
             three leptons are used, which are further categorized by the
             presence of boosted W, Z, and Higgs bosons and top quarks.
             The categorization is performed using a neural-network-based
             boosted object tagger to enhance the sensitivity to signal
             relative to the background. No significant excess above the
             background expectation is observed and exclusion limits at
             95% confidence level are set on the masses of the
             vector-like partners T and B of the top and bottom quarks,
             respectively. The limits depend on the branching ratio
             configurations and, in the case of 100% branching ratio for
             T→Zt and 100% branching ratio for B→Zb, this search sets
             the most stringent limits to date, allowing mT>1.60TeV and
             mB>1.42TeV, respectively.},
   Doi = {10.1016/j.physletb.2023.138019},
   Key = {fds372125}
}

@article{fds347451,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A},
   Title = {Search for pairs of highly collimated photon-jets in pp
             collisions at s =13 TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {99},
   Number = {1},
   Year = {2019},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.99.012008},
   Abstract = {Results of a search for the pair production of photon-jets -
             collimated groupings of photons - in the ATLAS detector at
             the Large Hadron Collider are reported. Highly collimated
             photon-jets can arise from the decay of new, highly boosted
             particles that can decay to multiple photons collimated
             enough to be identified in the electromagnetic calorimeter
             as a single, photonlike energy cluster. Data from
             proton-proton collisions at a center-of-mass energy of 13
             TeV, corresponding to an integrated luminosity of 36.7 fb-1,
             were collected in 2015 and 2016. Candidate photon-jet pair
             production events are selected from those containing two
             reconstructed photons using a set of identification criteria
             much less stringent than that typically used for the
             selection of photons, with additional criteria applied to
             provide improved sensitivity to photon-jets. Narrow excesses
             in the reconstructed diphoton mass spectra are searched for.
             The observed mass spectra are consistent with the Standard
             Model background expectation. The results are interpreted in
             the context of a model containing a new, high-mass scalar
             particle with narrow width, X, that decays into pairs of
             photon-jets via new, light particles, a. Upper limits are
             placed on the cross section times the product of branching
             ratios σ×B(X→aa)×B(a→γγ)2 for 200 GeV<mX<2 TeV and
             for ranges of ma from a lower mass of 100 MeV up to between
             2 and 10 GeV, depending upon mX. Upper limits are also
             placed on σ×B(X→aa)×B(a→3π0)2 for the same range of
             mX and for ranges of ma from a lower mass of 500 MeV up to
             between 2 and 10 GeV.},
   Doi = {10.1103/PhysRevD.99.012008},
   Key = {fds347451}
}

@article{fds373738,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
             J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
             Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
             GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
             M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
             JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
             C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
             KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
   Title = {Search for pairs of muons with small displacements in pp
             collisions at s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {846},
   Year = {2023},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.138172},
   Abstract = {A search for new phenomena giving rise to pairs of opposite
             electrically charged muons with impact parameters in the
             millimeter range is presented, using 139 fb−1 of s=13 TeV
             pp collision data from the ATLAS detector at the LHC. The
             search targets the gap in coverage between existing searches
             targeting final states with leptons with large displacement
             and prompt leptons. No significant excess over the
             background expectation is observed and exclusion limits are
             set on the mass of long-lived scalar supersymmetric
             muon-partners (smuons) with much lower lifetimes than
             previously targeted by displaced muon searches. Smuon
             lifetimes down to 1 ps are excluded for a smuon mass of 100
             GeV, and smuon masses up to 520 GeV are excluded for a
             proper lifetime of 10 ps, at 95% confidence level. Finally,
             model-independent limits are set on the contribution from
             new phenomena to the signal-region yields.},
   Doi = {10.1016/j.physletb.2023.138172},
   Key = {fds373738}
}

@article{fds353481,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {Search for pairs of scalar leptoquarks decaying into quarks
             and electrons or muons in √s = 13 TeV pp collisions with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {10},
   Year = {2020},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2020)112},
   Abstract = {A search for new-physics resonances decaying into a lepton
             and a jet performed by the ATLAS experiment is presented.
             Scalar leptoquarks pair-produced in pp collisions at s = 13
             TeV at the Large Hadron Collider are considered using an
             integrated luminosity of 139 fb−1, corresponding to the
             full Run 2 dataset. They are searched for in events with two
             electrons or two muons and two or more jets, including jets
             identified as arising from the fragmentation of c- or
             b-quarks. The observed yield in each channel is consistent
             with the Standard Model background expectation. Leptoquarks
             with masses below 1.8 TeV and 1.7 TeV are excluded in the
             electron and muon channels, respectively, assuming a
             branching ratio into a charged lepton and a quark of 100%,
             with minimal dependence on the quark flavour. Upper limits
             on the aforementioned branching ratio are also given as a
             function of the leptoquark mass. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP10(2020)112},
   Key = {fds353481}
}

@article{fds354612,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
             KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
   Title = {Search for phenomena beyond the Standard Model in events
             with large b-jet multiplicity using the ATLAS detector at
             the LHC},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {1},
   Year = {2021},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-08730-0},
   Abstract = {A search is presented for new phenomena in events
             characterised by high jet multiplicity, no leptons
             (electrons or muons), and four or more jets originating from
             the fragmentation of b-quarks (b-jets). The search uses
             139fb-1 of s = 13 TeV proton–proton collision data
             collected by the ATLAS experiment at the Large Hadron
             Collider during Run 2. The dominant Standard Model
             background originates from multijet production and is
             estimated using a data-driven technique based on an
             extrapolation from events with low b-jet multiplicity to the
             high b-jet multiplicities used in the search. No significant
             excess over the Standard Model expectation is observed and
             95% confidence-level limits that constrain simplified models
             of R-parity-violating supersymmetry are determined. The
             exclusion limits reach 950 GeV in top-squark mass in the
             models considered.},
   Doi = {10.1140/epjc/s10052-020-08730-0},
   Key = {fds354612}
}

@article{fds356707,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Arnaez, O and Arnold, H},
   Title = {Search for photonic signatures of gauge-mediated
             supersymmetry in 13 TeV pp collisions with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {97},
   Number = {9},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.97.092006},
   Abstract = {A search is presented for photonic signatures, motivated by
             generalized models of gauge-mediated supersymmetry breaking.
             This search makes use of proton-proton collision data at
             √s = 13 TeV corresponding to an integrated luminosity of
             36.1 fb-1 recorded by the ATLAS detector at the LHC, and it
             explores models dominated by both strong and electroweak
             production of supersymmetric partner states. Experimental
             signatures incorporating an isolated photon and significant
             missing transverse momentum are explored. These signatures
             include events with an additional photon or additional jet
             activity not associated with any specific underlying quark
             flavor. No significant excess of events is observed above
             the Standard Model prediction, and 95% confidence-level
             upper limits of between 0.083 and 0.32 fb are set on the
             visible cross section of contributions from physics beyond
             the Standard Model. These results are interpreted in terms
             of lower limits on the masses of gluinos, squarks, and
             gauginos in the context of generalized models of
             gauge-mediated supersymmetry, which reach as high as 2.3 TeV
             for strongly produced and 1.3 TeV for weakly produced
             supersymmetric partner pairs.},
   Doi = {10.1103/PhysRevD.97.092006},
   Key = {fds356707}
}

@article{fds313608,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for photonic signatures of gauge-mediated
             supersymmetry in 8 TeV pp collisions with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.072001},
   Abstract = {A search is presented for photonic signatures motivated by
             generalized models of gauge-mediated supersymmetry breaking.
             This search makes use of 20.3 fb-1 of proton-proton
             collision data at √s = 8 TeV recorded by the ATLAS
             detector at the LHC, and explores models dominated by both
             strong and electroweak production of supersymmetric partner
             states. Four experimental signatures incorporating an
             isolated photon and significant missing transverse momentum
             are explored. These signatures include events with an
             additional photon, lepton, b-quark jet, or jet activity not
             associated with any specific underlying quark flavor. No
             significant excess of events is observed above the Standard
             Model prediction and model-dependent 95% confidence-level
             exclusion limits are set.},
   Doi = {10.1103/PhysRevD.92.072001},
   Key = {fds313608}
}

@article{fds310299,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Search for production of an Υ (1 S) meson in association
             with a W or Z boson using the full 1.96 TeV pp ¯ collision
             data set at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.052011},
   Abstract = {Production of the Υ(1S) meson in association with a vector
             boson is a rare process in the standard model with a cross
             section predicted to be below the sensitivity of the
             Tevatron. Observation of this process could signify
             contributions not described by the standard model or reveal
             limitations with the current nonrelativistic
             quantum-chromodynamic models used to calculate the cross
             section. We perform a search for this process using the full
             Run II data set collected by the CDF II detector
             corresponding to an integrated luminosity of 9.4fb-1. The
             search considers the Υ→μμ decay and the decay of the W
             and Z bosons into muons and electrons. In these purely
             leptonic decay channels, we observe one ΥW candidate with
             an expected background of 1.2±0.5 events, and one ΥZ
             candidate with an expected background of 0.1±0.1 events.
             Both observations are consistent with the predicted
             background contributions. The resulting upper limits on the
             cross section for Υ+W/Z production are the most sensitive
             reported from a single experiment and place restrictions on
             potential contributions from non-standard-model
             physics.},
   Doi = {10.1103/PhysRevD.91.052011},
   Key = {fds310299}
}

@article{fds307846,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for Production of Heavy Particles Decaying to Top
             Quarks and Invisible Particles in $p\overline{p}$ Collisions
             at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {19},
   Pages = {191801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.191801},
   Abstract = {We present a search for a new particle T' decaying to top
             quark via T' → t + X, where X is an invisible particle. In
             a data sample with 4.8  fb(-1) of integrated luminosity
             collected by the CDF II detector at Fermilab in pp
             collisions with √s = 1.96  TeV, we search for pair
             production of T' in the lepton + jets channel, pp → tt + X
             + X → ℓνbqq'b + X + X. We interpret our results
             primarily in terms of a model where T' are exotic fourth
             generation quarks and X are dark matter particles. Current
             direct and indirect bounds on such exotic quarks restrict
             their masses to be between 300 and 600  GeV/c2, the dark
             matter particle mass being anywhere below m(T'). The data
             are consistent with standard model expectations, and we set
             95% confidence level limits on the generic production of
             T'T' → tt + X + X. For the dark matter model we exclude T'
             at 95% confidence level up to m(T') = 360  GeV/c2 for
             m(X) ≤ 100  GeV/c2.},
   Doi = {10.1103/PhysRevLett.106.191801},
   Key = {fds307846}
}

@article{fds307701,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten,
             K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benitez Garcia and JA and Benjamin, DP and Benoit,
             M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Search for production of resonant states in the photon-jet
             mass distribution using pp collisions at √s=7 TeV
             collected by the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {21},
   Pages = {211802},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.211802},
   Abstract = {This Letter describes a model-independent search for the
             production of new resonant states in photon+jet events in
             2.11 fb(-1) of proton-proton collisions at √s=7 TeV. We
             compare the photon+jet mass distribution to a background
             model derived from data and find consistency with the
             background-only hypothesis. Given the lack of evidence for a
             signal, we set 95% credibility level limits on generic
             Gaussian-shaped signals and on a benchmark excited-quark
             (q*) model, excluding 2 TeV Gaussian resonances with cross
             section times branching fraction times acceptance times
             efficiency near 5 fb and excluding q* masses below 2.46 TeV,
             respectively.},
   Doi = {10.1103/physrevlett.108.211802},
   Key = {fds307701}
}

@article{fds310268,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
             G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for production of vector-like quark pairs and of four
             top quarks in the lepton-plus-jets final state in pp
             collisions at √s = 8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2015)105},
   Abstract = {A search for pair production of vector-like quarks, both
             up-type (T) and down-type (B), as well as for four-top-quark
             production, is presented. The search is based on pp
             collisions at (Formula presented.) TeV recorded in 2012 with
             the ATLAS detector at the CERN Large Hadron Collider and
             corresponding to an integrated luminosity of 20.3 fb−1.
             Data are analysed in the lepton-plus-jets final state,
             characterised by an isolated electron or muon with high
             transverse momentum, large missing transverse momentum and
             multiple jets. Dedicated analyses are performed targeting
             three cases: a T quark with significant branching ratio to a
             W boson and a b-quark (TT¯→Wb+X), and both a T quark and
             a B quark with significant branching ratio to a Higgs boson
             and a third-generation quark (TT¯→Ht+XandBB¯→Hb+X
             respectively). No significant excess of events above the
             Standard Model expectation is observed, and 95% CL lower
             limits are derived on the masses of the vector-like T and B
             quarks under several branching ratio hypotheses assuming
             contributions from T → Wb, Zt, Ht and B → Wt, Zb, Hb
             decays. The 95% CL observed lower limits on the T quark mass
             range between 715 GeV and 950 GeV for all possible values of
             the branching ratios into the three decay modes, and are the
             most stringent constraints to date. Additionally, the most
             restrictive upper bounds on four-top-quark production are
             set in a number of new physics scenarios.},
   Doi = {10.1007/JHEP08(2015)105},
   Key = {fds310268}
}

@article{fds310319,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca,
             D and Cindro, V and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
             S},
   Title = {Search for production of [Formula: see text] resonances
             decaying to a lepton, neutrino and jets in [Formula: see
             text] collisions at [Formula: see text] TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {5},
   Pages = {209},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3425-6},
   Abstract = {A search is presented for narrow diboson resonances decaying
             to [Formula: see text] or [Formula: see text] in the final
             state where one [Formula: see text] boson decays
             leptonically (to an electron or a muon plus a neutrino) and
             the other [Formula: see text] boson decays hadronically. The
             analysis is performed using an integrated luminosity of
             20.3 fb[Formula: see text] of [Formula: see text]
             collisions at [Formula: see text] TeV collected by the
             ATLAS detector at the large hadron collider. No evidence for
             resonant diboson production is observed, and resonance
             masses below 700 and 1490 GeV are excluded at 95 %
             confidence level for the spin-2 Randall-Sundrum bulk
             graviton [Formula: see text] with coupling constant of 1.0
             and the extended gauge model [Formula: see text] boson
             respectively.},
   Doi = {10.1140/epjc/s10052-015-3425-6},
   Key = {fds310319}
}

@article{fds307547,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
             E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
             N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
             R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat,
             P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov,
             AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canelli, F and Canepa,
             A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin,
             V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba,
             J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B},
   Title = {Search for quantum black hole production in
             high-invariant-mass lepton+jet final states using pp
             collisions at √s=8  TeV and the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {9},
   Pages = {091804},
   Year = {2014},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.112.091804},
   Abstract = {This Letter presents a search for quantum black-hole
             production using 20.3 fb-1 of data collected with the ATLAS
             detector in pp collisions at the LHC at √s = 8 TeV. The
             quantum black holes are assumed to decay into a final state
             characterized by a lepton (electron or muon) and a jet. In
             either channel, no event with a lepton-jet invariant mass of
             3.5 TeV or more is observed, consistent with the expected
             background. Limits are set on the product of cross sections
             and branching fractions for the lepton+jet final states of
             quantum black holes produced in a search region for
             invariant masses above 1 TeV. The combined 95% confidence
             level upper limit on this product for quantum black holes
             with threshold mass above 3.5 TeV is 0.18 fb. This limit
             constrains the threshold quantum black-hole mass to be above
             5.3 TeV in the model considered.},
   Doi = {10.1103/physrevlett.112.091804},
   Key = {fds307547}
}

@article{fds376311,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
             L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V},
   Title = {Search for quantum black hole production in lepton + jet
             final states using proton-proton collisions at vs = 13 TeV
             with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {109},
   Number = {3},
   Year = {2024},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.109.032010},
   Abstract = {A search for quantum black holes in electron + jet and muon
             + jet invariant mass spectra is performed with 140 fb-1 of
             data collected by the ATLAS detector in proton-proton
             collisions at √s = 13 TeV at the Large Hadron Collider.
             The observed invariant mass spectrum of lepton + jet pairs
             is consistent with Standard Model expectations. Upper limits
             are set at 95% confidence level on the production cross
             section times branching fractions for quantum black holes
             decaying into a lepton and a quark in a search region with
             invariant mass above 2.0 TeV. The resulting quantum black
             hole lower mass threshold limit is 9.2 TeV in the
             Arkani-Hamed-Dimopoulos-Dvali model, and 6.8 TeV in the
             Randall-Sundrum model.},
   Doi = {10.1103/PhysRevD.109.032010},
   Key = {fds376311}
}

@article{fds308192,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
             A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
             C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson,
             R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin,
             T and Dittmann, JR and Dominguez, A and Donati, S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erbacher, R and Errede, D and Errede, S and Fan, Q and Feild,
             RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman,
             J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov, I and Goshaw,
             AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
             J and Heiss, A and Herndon, M and Hill, C and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
             T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kotwal, AV and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and IV, AML and Lee, K and Leone, S and Lewis,
             JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima,
             K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
             P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos,
             A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot,
             J and Ptohos, F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto,
             WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt,
             M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel,
             S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
             A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
             AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding,
             J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel,
             L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi, K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonelli, D and Toyoda,
             H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa,
             F and Vaiciulis, T and Valls, J and III, SV and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner, RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters,
             D and Watts, T and Webb, R and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Search for quark-lepton compositeness and a heavy W′ Boson
             using the eν channel in pp̄ Collisions at √s = 1.8
             TeV},
   Journal = {Physical Review Letters},
   Volume = {87},
   Number = {23},
   Pages = {2318031-2318036},
   Year = {2001},
   Month = {Winter},
   ISSN = {0031-9007},
   url = {http://www.ncbi.nlm.nih.gov/pubmed/11736446},
   Abstract = {A study on searches for quark-lepton compositeness and a
             heavy boson at high electron-neutrino transverse mass was
             presented. The data collected in pp̄ collisions at √s=1.8
             TeV was used for the analysis. The data obtained is found to
             be consistent with the standard model (SM)
             predictions.},
   Doi = {10.1103/physrevlett.87.231803},
   Key = {fds308192}
}

@article{fds331392,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evans, H and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk,
             HE and Fisyak, Y and Flattum, E},
   Title = {Search for R-parity violating supersymmetry in the
             dielectron channel},
   Journal = {Physical Review Letters},
   Volume = {83},
   Number = {22},
   Pages = {4476-4481},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.83.4476},
   Abstract = {We report on a search for R-parity-violating supersymmetry
             in pp¯ collisions at √=1.8TeV using the D0 detector at
             Fermilab. Events with at least two electrons and four or
             more jets were studied. We observe two events in
             99±4.4pb−1 of data, consistent with the expected
             background of 1.8±0.4 events. This result is interpreted
             within the framework of minimal low-energy supergravity
             supersymmetry models. Squarks with mass below 243 GeV/c2 and
             gluinos with mass below 227GeV/c2 are excluded at the 95%
             C.L. for A0 = 0, μ<0, tan β=2, and a finite value for any
             one of the six R-parity-violating couplings λ′1jk (j=1, 2
             and k=1, 2, 3). © 1999 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.83.4476},
   Key = {fds331392}
}

@article{fds308170,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon,
             TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
             VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
             F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Duperrin, A and Dyshkant, A and Edmunds, D and Ellison, J and Eltzroth, JT and Elvira, VD and Engelmann,
             R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein, D and Ferbel, T and Filthaut, F and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Fox, H and Frame, KC and Fu, S and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin, R and Ginther,
             G and Gómez, B and Gómez, G and Goncharov, PI and González Solís,
             JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Greenwood,
             ZD and Grinstein, S and Groer, L and Grünendahl, S and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinmiller, JM and Heinson, AP and Heintz, U and Hildreth, MD and Hirosky, R and Hobbs, JD and Hoeneisen, B and Huang, Y and Iashvili, I and Illingworth, R and Ito, AS and Jaffré, M and Jain, S and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jöstlein, H and Juste, A and Kahl, W and Kahn, S and Kajfasz, E and Kalinin, AM and Karmanov, D and Karmgard, D and Kehoe, R and Khanov, A and Kharchilava, A and Kim, SK and Klima, B and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kothari, B and Kotwal, AV and Kozelov, AV and Kozlovsky,
             EA and Krane, J and Krishnaswamy, MR and Krivkova, P and Krzywdzinski,
             S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kuznetsov, VE and Landsberg, G and Lee, WM and Leflat, A and Leggett, C and Lehner, F and Leonidopoulos, C and Li, J and Li, QZ and Li, X and Lima,
             JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lucotte,
             A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AKA and Madaras,
             RJ and Malyshev, VL and Manankov, V and Mao, HS and Marshall, T and Martin,
             MI and Mauritz, KM and Mayorov, AA and McCarthy, R and McMahon, T and Melanson, HL and Merkin, M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery,
             HE and Moore, RW and Mostafa, M and Da Motta and H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Naumann, NA and Neal, HA and Negret,
             JP and Negroni, S and Nunnemann, T and O'Neil, D and Oguri, V and Olivier,
             B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou, K and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Perkins, J and Peters, O and Pétroff, P and Piegaia, R and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Przybycien, MB and Qian, J and Raja, R and Rajagopalan, S and Ramberg,
             E and Rapidis, PA and Reay, NW and Reucroft, S and Ridel, M and Rijssenbeek, M and Rizatdinova, F and Rockwell, T and Roco, M and Royon,
             C and Rubinov, P and Ruchti, R and Rutherfoord, J and Sabirov, BM and Sajot, G and Santoro, A and Sawyer, L and Schamberger, RD and Schellman,
             H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell, RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery, P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Song,
             Y and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stichelbaut, F and Stoker, D and Stolin, V and Stone, A and Stoyanova,
             DA and Strang, MA and Strauss, M and Strovink, M and Stutte, L and Sznajder, A and Talby, M and Taylor, W and Tentindo-Repond, S and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and Vaniev, V and Van Kooten and R and Varelas, N and Vertogradov, LS and Villeneuve-Seguier, F and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, Z-M and Warchol, J and Watts, G and Wayne, M and Weerts,
             H and White, A and White, JT and Whiteson, D and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Womersley, J and Wood, DR and Xu, Q and Yamada, R and Yamin, P and Yasuda, T and Yatsunenko, YA and Yip, K and Youssef, S and Yu, J and Yu, Z and Zanabria, M and Zhang, X and Zheng, H and Zhou, B and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev, EG and Zylberstejn, A},
   Title = {Search for R-parity violating supersymmetry in two-muon and
             four-jet topologies.},
   Journal = {Physical review letters},
   Volume = {89},
   Number = {17},
   Pages = {171801},
   Year = {2002},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.89.171801},
   Abstract = {We present results of a search for R-parity-violating decay
             of the neutralino chi;01, taken as the lightest
             supersymmetric particle, to a muon and two jets. The decay
             proceeds through a lepton-number violating coupling
             lambda(')(2jk) (j=1,2; k=1,2,3), with R-parity conservation
             in all other production and decay processes. In the absence
             of candidate events from 77.5+/-3.9 pb(-1) of data collected
             by the D0 experiment at the Fermilab Tevatron in pp
             collisions at sqrt[s]=1.8 TeV, and with an expected
             background of 0.18+/-0.03+/-0.02 events, we set limits on
             squark and gluino masses within the framework of the minimal
             low-energy supergravity-supersymmetry model.},
   Doi = {10.1103/physrevlett.89.171801},
   Key = {fds308170}
}

@article{fds308204,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bean, A and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar,
             V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler,
             M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl,
             OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov,
             D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann,
             R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein,
             D},
   Title = {Search for R-parity violation in multilepton final states in
             [formula presented] collisions at [formula
             presented]},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {62},
   Number = {7},
   Pages = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.62.071701},
   Abstract = {The result of a search for gaugino pair production with a
             trilepton signature is reinterpreted in the framework of
             minimal supergravity (MSUGRA) with R-parity violation via
             leptonic λ Yukawa couplings. The search used 95 (Formula
             presented) of (Formula presented) collisions at (Formula
             presented) recorded by the DØ detector at the Fermilab
             Tevatron. A large domain of the MSUGRA parameter space is
             excluded for (Formula presented) (Formula presented). ©
             2000 The American Physical Society.},
   Doi = {10.1103/PhysRevD.62.071701},
   Key = {fds308204}
}

@article{fds356652,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
             M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G},
   Title = {Search for R-parity-violating supersymmetric particles in
             multi-jet final states produced in p–p collisions at s=13
             TeV using the ATLAS detector at the LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {785},
   Pages = {136-158},
   Year = {2018},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.08.021},
   Abstract = {Results of a search for gluino pair production with
             subsequent R-parity-violating decays to quarks are
             presented. This search uses 36.1 fb−1 of data collected by
             the ATLAS detector in proton–proton collisions with a
             centre-of-mass energy of s=13 TeV at the LHC. The analysis
             is performed using requirements on the number of jets and
             the number of jets tagged as containing a b-hadron as well
             as a topological observable formed by the scalar sum of
             masses of large-radius jets in the event. No significant
             excess above the expected Standard Model background is
             observed. Limits are set on the production of gluinos in
             models with the R-parity-violating decays of either the
             gluino itself (direct decay) or the neutralino produced in
             the R-parity-conserving gluino decay (cascade decay). In the
             gluino cascade decay model, gluino masses below 1850 GeV are
             excluded for 1000 GeV neutralino mass. For the gluino direct
             decay model, the 95% confidence level upper limit on the
             cross section times branching ratio varies between 0.80 fb
             at mg˜=900 GeV and 0.011 fb at mg˜=1800
             GeV.},
   Doi = {10.1016/j.physletb.2018.08.021},
   Key = {fds356652}
}

@article{fds359998,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
             J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
             C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce,
             ATH and Arena, E and Arguin, JF and Argyropoulos, S and Arling,
             JH},
   Title = {Search for R-parity-violating supersymmetry in a final state
             containing leptons and many jets with the ATLAS experiment
             using √s=13TeV proton–proton collision
             data},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {11},
   Year = {2021},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09761-x},
   Abstract = {A search for R-parity-violating supersymmetry in final
             states characterized by high jet multiplicity, at least one
             isolated light lepton and either zero or at least three
             b-tagged jets is presented. The search uses 139fb-1 of
             s=13TeV proton–proton collision data collected by the
             ATLAS experiment during Run 2 of the Large Hadron Collider.
             The results are interpreted in the context of
             R-parity-violating supersymmetry models that feature gluino
             production, top-squark production, or electroweakino
             production. The dominant sources of background are estimated
             using a data-driven model, based on observables at medium
             jet multiplicity, to predict the b-tagged jet multiplicity
             distribution at the higher jet multiplicities used in the
             search. Machine-learning techniques are used to reach
             sensitivity to electroweakino production, extending the
             data-driven background estimation to the shape of the
             machine-learning discriminant. No significant excess over
             the Standard Model expectation is observed and exclusion
             limits at the 95% confidence level are extracted, reaching
             as high as 2.4 TeV in gluino mass, 1.35 TeV in top-squark
             mass, and 320 (365) GeV in higgsino (wino)
             mass.},
   Doi = {10.1140/epjc/s10052-021-09761-x},
   Key = {fds359998}
}

@article{fds307664,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for R-parity-violating supersymmetry in events with
             four or more leptons in √s =7 TeV pp collisions with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {12},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2012)124},
   Abstract = {A search for new phenomena in final states with four or more
             leptons (electrons or muons) is presented. The analysis is
             based on 4.7 fb-1 of √s =7 TeV proton-proton collisions
             delivered by the Large Hadron Collider and recorded with the
             ATLAS detector. Observations are consistent with Standard
             Model expectations in two signal regions: one that requires
             moderate values of missing transverse momentum and another
             that requires large effective mass. The results are
             interpreted in a simplified model of R-parity-violating
             supersymmetry in which a 95% CL exclusion region is set for
             charged wino masses up to 540 GeV. In an R-parity-violating
             MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are
             excluded for 10 < tan β < 40. © 2012 Cern for the benefit
             of the ATLAS collaboration.},
   Doi = {10.1007/JHEP12(2012)124},
   Key = {fds307664}
}

@article{fds356534,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {Search for resonances decaying into a weak vector boson and
             a Higgs boson in the fully hadronic final state produced in
             proton-proton collisions at s =13 TeV with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {102},
   Number = {11},
   Year = {2020},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.102.112008},
   Abstract = {A search for heavy resonances decaying into a W or Z boson
             and a Higgs boson produced in proton-proton collisions at
             the Large Hadron Collider at s=13 TeV is presented. The
             analysis utilizes the dominant W→qq¯′ or Z→qq¯ and
             H→bb¯ decays with substructure techniques applied to
             large-radius jets. A sample corresponding to an integrated
             luminosity of 139 fb-1 collected with the ATLAS detector is
             analyzed and no significant excess of data is observed over
             the background prediction. The results are interpreted in
             the context of the heavy vector triplet model with spin-1
             W′ and Z′ bosons. Upper limits on the cross section are
             set for resonances with mass between 1.5 and 5.0 TeV,
             ranging from 6.8 to 0.53 fb for W′→WH and from 8.7 to
             0.53 fb for Z′→ZH at the 95% confidence
             level.},
   Doi = {10.1103/PhysRevD.102.112008},
   Key = {fds356534}
}

@article{fds307644,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for resonances decaying into top-quark pairs using
             fully hadronic decays in pp collisions with ATLAS at √s=7
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP01(2013)116},
   Abstract = {A search for resonances produced in 7 TeV proton-proton
             collisions and decaying into top-quark pairs is described.
             In this Letter events where the top-quark decay produces two
             massive jets with large transverse momenta recorded with the
             ATLAS detector at the Large Hadron Collider are considered.
             Two techniques that rely on jet substructure are used to
             separate top-quark jets from those arising from light quarks
             and gluons. In addition, each massive jet is required to
             have evidence of an associated bottom-quark decay. The data
             are consistent with the Standard Model, and limits can be
             set on the production cross section times branching fraction
             of a Z′ boson and a Kaluza-Klein gluon resonance. These
             limits exclude, at the 95% credibility level, Z′ bosons
             with masses 0.70-1.00 TeV as well as 1.28-1.32 TeV and
             Kaluza-Klein gluons with masses 0.70-1.62 TeV. © 2013 Cern
             for the benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP01(2013)116},
   Key = {fds307644}
}

@article{fds310264,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Anzà, F and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
             A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bianchi, L and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
             J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino,
             P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon,
             CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat,
             P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano,
             I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino,
             G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos,
             F and Punzi, G and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
             J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St
             Denis, R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
             P and Wallny, R and Wang, SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Search for Resonances Decaying to Top and Bottom Quarks with
             the CDF Experiment.},
   Journal = {Physical review letters},
   Volume = {115},
   Number = {6},
   Pages = {061801},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.115.061801},
   Abstract = {We report on a search for charged massive resonances
             decaying to top (t) and bottom (b) quarks in the full data
             set of proton-antiproton collisions at a center-of-mass
             energy of √[s]=1.96  TeV collected by the CDF II
             detector at the Tevatron, corresponding to an integrated
             luminosity of 9.5  fb(-1). No significant excess above
             the standard model background prediction is observed. We set
             95% Bayesian credibility mass-dependent upper limits on the
             heavy charged-particle production cross section times
             branching ratio to tb. Using a standard model extension with
             a W'→tb and left-right-symmetric couplings as a benchmark
             model, we constrain the W' mass and couplings in the
             300-900  GeV/c(2) range. The limits presented here are
             the most stringent for a charged resonance with mass in the
             range 300-600  GeV/c(2) decaying to top and bottom
             quarks.},
   Doi = {10.1103/physrevlett.115.061801},
   Key = {fds310264}
}

@article{fds321091,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Search for resonances in diphoton events at √s=13 TeV with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2016)001},
   Abstract = {Searches for new resonances decaying into two photons in the
             ATLAS experiment at the CERN Large Hadron Collider are
             described. The analysis is based on proton-proton collision
             data corresponding to an integrated luminosity of 3.2 fb−1
             at s=13 TeV recorded in 2015. Two searches are performed,
             one targeted at a spin-2 particle of mass larger than 500
             GeV, using Randall-Sundrum graviton states as a benchmark
             model, and one optimized for a spin-0 particle of mass
             larger than 200 GeV. Varying both the mass and the decay
             width, the most significant deviation from the
             background-only hypothesis is observed at a diphoton
             invariant mass around 750 GeV with local significances of
             3.8 and 3.9 standard deviations in the searches optimized
             for a spin-2 and spin-0 particle, respectively. The global
             significances are estimated to be 2.1 standard deviations
             for both analyses. The consistency between the data
             collected at 13 TeV and 8 TeV is also evaluated. Limits on
             the production cross section times branching ratio to two
             photons for the two resonance types are reported.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP09(2016)001},
   Key = {fds321091}
}

@article{fds356671,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
   Title = {Search for resonances in the mass distribution of jet pairs
             with one or two jets identified as b -jets in proton-proton
             collisions at s =13 TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {3},
   Year = {2018},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.032016},
   Abstract = {A search for new resonances decaying into jets containing
             b-hadrons in pp collisions with the ATLAS detector at the
             LHC is presented in the dijet mass range from 0.57 to 7 TeV.
             The data set corresponds to an integrated luminosity of up
             to 36.1 fb-1 collected in 2015 and 2016 at s=13 TeV. No
             evidence of a significant excess of events above the smooth
             background shape is found. Upper cross-section limits and
             lower limits on the corresponding signal mass parameters for
             several types of signal hypotheses are provided at 95% C.L.
             In addition, 95% C.L. upper limits are set on the cross
             sections for new processes that would produce
             Gaussian-shaped signals in the di-b-jet mass
             distributions.},
   Doi = {10.1103/PhysRevD.98.032016},
   Key = {fds356671}
}

@article{fds321131,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for resonances in the mass distribution of jet pairs
             with one or two jets identified as b-jets in proton–proton
             collisions at s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {759},
   Pages = {229-246},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.05.064},
   Abstract = {Searches for high-mass resonances in the dijet invariant
             mass spectrum with one or two jets identified as b-jets are
             performed using an integrated luminosity of 3.2 fb−1 of
             proton–proton collisions with a centre-of-mass energy of
             s=13 TeV recorded by the ATLAS detector at the Large Hadron
             Collider. No evidence of anomalous phenomena is observed in
             the data, which are used to exclude, at 95% credibility
             level, excited b⁎ quarks with masses from 1.1 TeV to 2.1
             TeV and leptophobic Z′ bosons with masses from 1.1 TeV to
             1.5 TeV. Contributions of a Gaussian signal shape with
             effective cross sections ranging from approximately 0.4 to
             0.001 pb are also excluded in the mass range 1.5–5.0
             TeV.},
   Doi = {10.1016/j.physletb.2016.05.064},
   Key = {fds321131}
}

@article{fds347454,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
             M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
             E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
             M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RMB and Biebel, O and Biedermann, D and Bielski,
             R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz,
             T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
             KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
             U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
             PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
             TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
             BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
             S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
             K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
             V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară,
             IA},
   Title = {Search for Resonant and Nonresonant Higgs Boson Pair
             Production in the bb[over ¯]τ^{+}τ^{-} Decay Channel in
             pp Collisions at sqrt[s]=13  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {121},
   Number = {19},
   Pages = {191801},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.121.191801},
   Abstract = {A search for resonant and nonresonant pair production of
             Higgs bosons in the bb[over ¯]τ^{+}τ^{-} final state is
             presented. The search uses 36.1  fb^{-1} of pp collision
             data with sqrt[s]=13  TeV recorded by the ATLAS
             experiment at the LHC in 2015 and 2016. Decays of the
             τ-lepton pairs with at least one τ lepton decaying to
             final states with hadrons and a neutrino are considered. No
             significant excess above the expected background is observed
             in the data. The cross-section times branching ratio for
             nonresonant Higgs boson pair production is constrained to be
             less than 30.9 fb, 12.7 times the standard model
             expectation, at 95% confidence level. The data are also
             analyzed to probe resonant Higgs boson pair production,
             constraining a model with an extended Higgs sector based on
             two doublets and a Randall-Sundrum bulk graviton model.
             Upper limits are placed on the resonant Higgs boson pair
             production cross-section times branching ratio, excluding
             resonances X in the mass range 305  GeV<m_{X}<402  GeV
             in the simplified hMSSM minimal supersymmetric model for
             tanβ=2 and excluding bulk Randall-Sundrum gravitons G_{KK}
             in the mass range 325  GeV<m_{G_{KK}}<885  GeV for
             k/M[over ¯]_{Pl}=1.},
   Doi = {10.1103/physrevlett.121.191801},
   Key = {fds347454}
}

@article{fds307595,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Search for resonant diboson production in the WW/WZ →
             ℓvjj decay channels with the ATLAS detector at √s = 7
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.112006},
   Abstract = {A search for resonant diboson production using a data sample
             corresponding to 4:7 fb–1of integrated luminosity
             collected by the ATLAS experiment at the Large Hadron
             Collider in pp collisions at √s = 7 TeV is presented. The
             search for a narrow resonance in the WW or WZ mass
             distribution is conducted in a final state with an electron
             or a muon, missing transverse momentum, and at least two
             jets. No significant excess is observed and limits are set
             using three benchmark models: WW resonance masses below 940
             and 710 GeV are excluded at 95% confidence level for spin-2
             Randall–Sundrum and bulk Randall–Sundrum gravitons,
             respectively; WZ resonance masses below 950 GeV are excluded
             at 95% confidence level for a spin-1 extended gauge model
             W′ boson.},
   Doi = {10.1103/PhysRevD.87.112006},
   Key = {fds307595}
}

@article{fds346165,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
             O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
             V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro,
             A},
   Title = {Search for resonant diboson production in the [Formula: see
             text] final state in [Formula: see text] collisions at
             [Formula: see text] TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {2},
   Pages = {69},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3261-8},
   Abstract = {This paper reports on a search for narrow resonances in
             diboson production in the [Formula: see text] final state
             using [Formula: see text] collision data corresponding to an
             integrated luminosity of [Formula: see text] fb[Formula:
             see text] collected at [Formula: see text] TeV with the
             ATLAS detector at the Large Hadron Collider. No significant
             excess of data events over the Standard Model expectation is
             observed. Upper limits at the 95 % confidence level are set
             on the production cross section times branching ratio for
             Kaluza-Klein gravitons predicted by the Randall-Sundrum
             model and for Extended Gauge Model [Formula: see text]
             bosons. These results lead to the exclusion of mass values
             below 740 and 1590 GeV for the graviton and [Formula: see
             text] boson respectively.},
   Doi = {10.1140/epjc/s10052-015-3261-8},
   Key = {fds346165}
}

@article{fds307871,
   Author = {Aaltonen, TEA},
   Title = {Search for resonant production of $t\overline{t}$ decaying
             to jets in $p\overline{p}$ collisions at
             $\sqrt{s}\mathbf{=}1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {7},
   Pages = {072003},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.072003},
   Abstract = {This paper reports a search for nonstandard model topquark
             resonances, Z′, decaying to tt̄→W+bW -b̄, where both W
             decay to quarks. We examine the top-antitop quark invariant
             mass spectrum for the presence of narrow resonant states.
             The search uses a data sample of pp̄ collisions at a center
             of mass energy of 1.96 TeV collected by the CDF II detector
             at the Fermilab Tevatron, with an integrated luminosity of
             2.8fb-1. No evidence for top-antitop quark resonant
             production is found. We place upper limits on the production
             cross section times branching ratio for a specific topcolor
             assisted technicolor model in which the Z′ has a width of
             Γ Z′=0.012MZ′. Within this model, we exclude a Z′
             boson with masses below 805GeV/c2 at the 95% confidence
             level. © 2011 American Physical Society.},
   Doi = {10.1103/PhysRevD.84.072003},
   Key = {fds307871}
}

@article{fds307872,
   Author = {Aaltonen, TEA},
   Title = {Search for resonant production of $t\overline{t}$ pairs in
             $4.8{\,}{\,}{\mathrm{fb}}^{\mathbf{-}1}$ of integrated
             luminosity of $p\overline{p}$ collisions at
             $\sqrt{s}\mathbf{=}1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {7},
   Pages = {072004},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.072004},
   Abstract = {We search for resonant production of tt̄ pairs in 4.8fb-1
             integrated luminosity of pp̄ collision data at √s=1.96TeV
             in the lepton+jets decay channel, where one top quark decays
             leptonically and the other hadronically. A matrix-element
             reconstruction technique is used; for each event a
             probability density function of the tt̄ candidate invariant
             mass is sampled. These probability density functions are
             used to construct a likelihood function, whereby the cross
             section for resonant tt̄ production is estimated, given a
             hypothetical resonance mass and width. The data indicate no
             evidence of resonant production of tt̄ pairs. A benchmark
             model of leptophobic Z′→tt̄ is excluded with m
             Z′<900GeV/c2 at 95% confidence level. © 2011 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.84.072004},
   Key = {fds307872}
}

@article{fds307665,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ},
   Title = {Search for resonant top quark plus jet production in
             tt̄+jets events with the ATLAS detector in pp collisions at
             √s=7TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.091103},
   Abstract = {This paper presents a search for a new heavy particle
             produced in association with a top or antitop quark. Two
             models in which the new heavy particle is a color singlet or
             a color triplet are considered, decaying, respectively, to
             t̄q or tq, leading to a resonance within the tt̄+jets
             signature. The full 2011 ATLAS pp collision data set from
             the LHC (4.7fb -1) is used to search for tt̄ events
             produced in association with jets, in which one of the W
             bosons from the top quarks decays leptonically and the other
             decays hadronically. The data are consistent with the
             Standard Model expectation, and a new particle with mass
             below 430 Gev for both W ′ boson and color triplet models
             is excluded at 95% confidence level, assuming unit
             right-handed coupling. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.86.091103},
   Key = {fds307665}
}

@article{fds307608,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and d'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
             P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu,
             C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes,
             L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
             C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
             K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
             J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
             P and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson,
             JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Search for resonant top-antitop production in the lepton
             plus jets decay mode using the full CDF data
             set.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {12},
   Pages = {121802},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.110.121802},
   Abstract = {This Letter reports a search for a narrow resonant state
             decaying into two W bosons and two b quarks where one W
             boson decays leptonically and the other decays into a
             quark-antiquark pair. The search is particularly sensitive
             to top-antitop resonant production. We use the full data
             sample of proton-antiproton collisions at a center-of-mass
             energy of 1.96 TeV collected by the CDF II detector at the
             Fermilab Tevatron, corresponding to an integrated luminosity
             of 9.45 fb(-1). No evidence for resonant production is
             found, and upper limits on the production cross section
             times branching ratio for a narrow resonant state are
             extracted. Within a specific benchmark model, we exclude a
             Z' boson with mass, M(Z'), below 915 GeV/c(2) decaying into
             a top-antitop pair at the 95% credibility level assuming a
             Z' boson decay width of Γ(Z') = 0.012 M(Z'). This is the
             most sensitive search for a narrow qq-initiated tt resonance
             in the mass region below 750 GeV/c(2).},
   Doi = {10.1103/physrevlett.110.121802},
   Key = {fds307608}
}

@article{fds356632,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
   Title = {Search for resonant WZ production in the fully leptonic
             final state in proton–proton collisions at s=13TeV with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {787},
   Pages = {68-88},
   Year = {2018},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.10.021},
   Abstract = {A search for a heavy resonance decaying into WZ in the fully
             leptonic channel (electrons and muons) is performed. It is
             based on proton–proton collision data collected by the
             ATLAS experiment at the Large Hadron Collider at a
             centre-of-mass energy of 13 TeV, corresponding to an
             integrated luminosity of 36.1 fb−1. No significant excess
             is observed over the Standard Model predictions and limits
             are set on the production cross section times branching
             ratio of a heavy vector particle produced either in
             quark–antiquark fusion or through vector-boson fusion.
             Constraints are also obtained on the mass and couplings of a
             singly charged Higgs boson, in the Georgi–Machacek model,
             produced through vector-boson fusion.},
   Doi = {10.1016/j.physletb.2018.10.021},
   Key = {fds356632}
}

@article{fds372217,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
             CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
             P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
             C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev,
             V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
             JF},
   Title = {Search for resonant WZ production in the fully leptonic
             final state in proton–proton collisions at √s=13 TeV
             with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {7},
   Year = {2023},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11437-7},
   Abstract = {A search for a WZ resonance, in the fully leptonic final
             state (electrons or muons), is performed using 139 fb - 1
             of data collected at a centre-of-mass energy of 13 TeV by
             the ATLAS detector at the Large Hadron Collider. The results
             are interpreted in terms of a singly charged Higgs boson of
             the Georgi–Machacek model, produced by WZ fusion, and of a
             Heavy Vector Triplet, with the resonance produced by WZ
             fusion or the Drell–Yan process. No significant excess
             over the Standard Model prediction is observed and limits
             are set on the production cross-section times branching
             ratio as a function of the resonance mass for these
             processes.},
   Doi = {10.1140/epjc/s10052-023-11437-7},
   Key = {fds372217}
}

@article{fds310405,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Search for resonant WZ production in the WZ → ℓνℓ′
             ℓ ′ channel in √ (s) = 7 TeV pp collisions with the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {June},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.112012},
   Abstract = {A generic search is presented for a heavy particle decaying
             to WZ → ℓν′ ℓ ′ (ℓ, ℓ′ = e, μ)final
             states. The data were recorded by the ATLAS detector in
             ffiffiffis √ s = 7 TeV pp collisions at the Large Hadron
             Collider and correspond to an integrated luminosity of 1:02
             fb-1. The transverse mass distribution of the selected WZ
             candidates is found to be consistent with the standard model
             expectation. Upper limits on the production cross section
             times branching ratio are derived using two benchmark models
             predicting a heavy particle decaying to a WZ
             pair.},
   Doi = {10.1103/PhysRevD.85.112012},
   Key = {fds310405}
}

@article{fds310310,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V},
   Title = {Search for s-channel single top-quark production in
             proton-proton collisions at √s=8 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {740},
   Pages = {118-136},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.11.042},
   Abstract = {This Letter presents a search at the LHC for s-channel
             single top-quark production in proton-proton collisions at a
             centre-of-mass energy of 8 TeV. The analyzed data set was
             recorded by the ATLAS detector and corresponds to an
             integrated luminosity of 20.3 fb-1. Selected events contain
             one charged lepton, large missing transverse momentum and
             exactly two b-tagged jets. A multivariate event classifier
             based on boosted decision trees is developed to discriminate
             s-channel single top-quark events from the main background
             contributions. The signal extraction is based on a binned
             maximum-likelihood fit of the output classifier
             distribution. The analysis leads to an upper limit on the
             s-channel single top-quark production cross-section of 14.6
             pb at the 95% confidence level. The fit gives a
             cross-section of σs = 5.0 ± 4.3 pb, consistent with the
             Standard Model expectation.},
   Doi = {10.1016/j.physletb.2014.11.042},
   Key = {fds310310}
}

@article{fds307534,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
             JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
             A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
             C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
             L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Vázquez, F and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Search for s-channel single-top-quark production in events
             with missing energy plus jets in pp collisions at sqrt[s] =
             1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {23},
   Pages = {231805},
   Year = {2014},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.112.231805},
   Abstract = {The first search for single-top-quark production from the
             exchange of an s-channel virtual W boson using events with
             an imbalance in the total transverse energy, b-tagged jets,
             and no identified leptons is presented. Assuming the
             electroweak production of top quarks of mass 172.5 GeV/c(2)
             in the s channel, a cross section of 1.12(-0.57)(+0.61)
             (stat+syst) pb with a significance of 1.9 standard
             deviations is measured. This measurement is combined with
             the result obtained from events with an imbalance in total
             transverse momentum, b-tagged jets, and exactly one
             identified lepton, yielding a cross section of
             1.36(-0.32)(+0.37) (stat+syst) pb, with a significance of
             4.2 standard deviations.},
   Doi = {10.1103/physrevlett.112.231805},
   Key = {fds307534}
}

@article{fds307773,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonak, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Search for same-sign top-quark production and
             fourth-generation down-type quarks in pp collisions at √s
             = 7 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {4},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2012)069},
   Abstract = {A search is presented for same-sign top-quark production and
             down-type heavy quarks of charge -1/3 in events with two
             isolated leptons (e or μ) that have the same electric
             charge, at least two jets and large missing transverse
             momentum. The data are selected from pp collisions at ps = 7
             TeV recorded by the ATLAS detector and correspond to an
             integrated luminosity of 1.04 fb-1. The observed data are
             consistent with expectations from Standard Model processes.
             Upper limits are set at 95% confidence level on the cross
             section of new sources of same-sign top-quark pair
             production of 1.4-2.0 pb depending on the assumed mediator
             mass. Upper limits are also set on the pair-production
             cross-section for new heavy down-type quarks; a lower limit
             of 450 GeV is set at 95% confidence level on the mass of
             heavy down-type quarks under the assumption that they decay
             100% of the time to Wt. Copyright CERN.},
   Doi = {10.1007/JHEP04(2012)069},
   Key = {fds307773}
}

@article{fds307706,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati,
             S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard,
             R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli,
             F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji,
             W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi,
             M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B},
   Title = {Search for scalar bottom quark pair production with the
             ATLAS detector in pp collisions at sqrt[s]=7  TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {18},
   Pages = {181802},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.181802},
   Abstract = {The results of a search for pair production of the scalar
             partners of bottom quarks in 2.05  fb(-1) of pp
             collisions at sqrt[s]=7  TeV using the ATLAS experiment
             are reported. Scalar bottom quarks are searched for in
             events with large missing transverse momentum and two jets
             in the final state, where both jets are identified as
             originating from a bottom quark. In an R-parity conserving
             minimal supersymmetric scenario, assuming that the scalar
             bottom quark decays exclusively into a bottom quark and a
             neutralino, 95% confidence-level upper limits are obtained
             in the b(1) - χ(1)(0) mass plane such that for neutralino
             masses below 60 GeV scalar bottom masses up to 390 GeV are
             excluded.},
   Doi = {10.1103/physrevlett.108.181802},
   Key = {fds307706}
}

@article{fds310288,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C},
   Title = {Search for Scalar Charm Quark Pair Production in pp
             Collisions at sqrt[s]=8  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {16},
   Pages = {161801},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.114.161801},
   Abstract = {The results of a dedicated search for pair production of
             scalar partners of charm quarks are reported. The search is
             based on an integrated luminosity of 20.3  fb^{-1} of pp
             collisions at sqrt[s]=8  TeV recorded with the ATLAS
             detector at the LHC. The search is performed using events
             with large missing transverse momentum and at least two
             jets, where the two leading jets are each tagged as
             originating from c quarks. Events containing isolated
             electrons or muons are vetoed. In an R-parity-conserving
             minimal supersymmetric scenario in which a single
             scalar-charm state is kinematically accessible, and where it
             decays exclusively into a charm quark and a neutralino, 95%
             confidence-level upper limits are obtained in the
             scalar-charm-neutralino mass plane such that, for neutralino
             masses below 200 GeV, scalar-charm masses up to 490 GeV
             are excluded.},
   Doi = {10.1103/physrevlett.114.161801},
   Key = {fds310288}
}

@article{fds310350,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Akesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
   Title = {Search for scalar diphoton resonances in the mass range
             65-600 GeV with the ATLAS detector in pp collision data at
             √s=8 TeV.},
   Journal = {Physical review letters},
   Volume = {113},
   Number = {17},
   Pages = {171801},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.113.171801},
   Abstract = {A search for scalar particles decaying via narrow resonances
             into two photons in the mass range 65-600 GeV is performed
             using 20.3  fb(-1) of √s 8 TeV pp collision data
             collected with the ATLAS detector at the Large Hadron
             Collider. The recently discovered Higgs boson is treated as
             a background. No significant evidence for an additional
             signal is observed. The results are presented as limits at
             the 95% confidence level on the production cross section of
             a scalar boson times branching ratio into two photons, in a
             fiducial volume where the reconstruction efficiency is
             approximately independent of the event topology. The upper
             limits set extend over a considerably wider mass range than
             previous searches.},
   Doi = {10.1103/physrevlett.113.171801},
   Key = {fds310350}
}

@booklet{Abbott97a,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
             V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
             C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
             P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
             MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
             G and Fisk, HE and Fisyak, Y and Flattum, E},
   Title = {Search for scalar leptoquark pairs decaying to electrons and
             jets in p®p collisions},
   Journal = {Physical Review Letters},
   Volume = {79},
   Number = {22},
   Pages = {4321-4326},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.4321},
   Abstract = {We have searched for the pair production of first generation
             scalar leptoquarks in the eejj channel using the full data
             set (123pb−1) collected with the D0 detector at the
             Fermilab Tevatron during 1992-1996. We observe no candidates
             with an expected background of approximately 0.4 events.
             Comparing the experimental 95% confidence level upper limit
             to theoretical calculations of the cross section with the
             assumption of a 100% branching fraction of eq, we set a
             lower limit on the mass of a first generation scalar
             leptoquark of 225 GeV/c2. The results of this analysis rule
             out the interpretation of the excess of high Q2 events at
             DESY HERA as leptoquarks which decay exclusively to eq. ©
             1997 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.79.4321},
   Key = {Abbott97a}
}

@article{fds308155,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
             J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri,
             A and Cerrito, L and Chapman, J and Chen, YC and Chertok, M and Chiarelli,
             G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chuang, S and Chung, K and Chung, WH and Chung, YS and Cijliak, M and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway,
             J},
   Title = {Search for scalar leptoquark pairs decaying to νν̄qq̄ in
             pp̄ collisions at s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {11},
   Pages = {1-7},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.112001},
   Abstract = {We report on a search for the pair production of scalar
             leptoquarks (LQ), using 191pb-1 of proton-antiproton
             collision data recorded by the CDF experiment during Run II
             of the Tevatron. The leptoquarks are sought via their decay
             into a neutrino and quark yielding missing transverse energy
             and several jets of large transverse energy. No evidence for
             LQ production is observed, and limits are set on
             σ(pp̄→LQLQ̄X→νν̄qq̄X). Using a next-to-leading
             order theoretical prediction of the cross section for LQ
             production, we exclude first-generation LQ in the mass
             interval 78 to 117GeV/c2 at the 95% confidence level for
             BR(LQ→νq)=100%. © 2005 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.71.112001},
   Key = {fds308155}
}

@article{fds321090,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for scalar leptoquarks in pp collisions at √S =
             13TeV with the ATLAS experiment},
   Journal = {New Journal of Physics},
   Volume = {18},
   Number = {9},
   Pages = {1-25},
   Publisher = {IOP Publishing},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1367-2630/18/9/093016},
   Abstract = {An inclusive search for a new-physics signature of
             lepton-jet resonances has been performed by the ATLAS
             experiment. Scalar leptoquarks, pair-produced in pp
             collisions at s √S13 TeV at the large hadron collider,
             have been considered. An integrated luminosity of 3.2
             fb−1, corresponding to the full 2015 dataset was used.
             First (second) generation leptoquarks were sought in events
             with two electrons (muons) and two or more jets. The
             observed event yield in each channel is consistent with
             Standard Model background expectations. The observed
             (expected) lower limits on the leptoquark mass at 95%
             confidence level are 1100 and 1050 GeV (1160 and 1040 GeV)
             for first and second generation leptoquarks, respectively,
             assuming a branching ratio into a charged lepton and a quark
             of 100%. Upper limits on the aforementioned branching ratio
             are also given as a function of leptoquark mass. Compared
             with the results of earlier ATLAS searches, the sensitivity
             is increased for leptoquark masses above 860 GeV, and the
             observed exclusion limits confirm and extend the published
             results.},
   Doi = {10.1088/1367-2630/18/9/093016},
   Key = {fds321090}
}

@article{fds356588,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA},
   Title = {Search for scalar resonances decaying into μ +
             μ  in events with and without b-tagged jets
             produced in proton-proton collisions at √s=13 TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {7},
   Year = {2019},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2019)117},
   Abstract = {A search for a narrow scalar resonance decaying into an
             opposite-sign muon pair produced in events with and without
             b-tagged jets is presented in this paper. The search uses
             36.1 fb−1 of s=13 TeV proton-proton collision data
             recorded by the ATLAS experiment at the LHC. No significant
             excess of events above the expected Standard Model
             background is observed in the investigated mass range of 0.2
             to 1.0 TeV. The observed upper limits at 95% confidence
             level on the cross section times branching ratio for b-quark
             associated production and gluon-gluon fusion are between 1.9
             and 41 fb and 1.6 and 44 fb respectively, which is
             consistent with expectations.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP07(2019)117},
   Key = {fds356588}
}

@article{fds307791,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós,
             G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber,
             T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz,
             SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet,
             NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Booth,
             CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
             P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom,
             PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni,
             G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
             M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
             T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins, NJ and Collins-Tooth, C and Collot,
             J and Colon, G and Muiño, PC and Coniavitis, E and Conidi,
             MC},
   Title = {Search for scalar top quark pair production in natural gauge
             mediated supersymmetry models with the ATLAS detector in pp
             collisions at s=7TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {715},
   Number = {1-3},
   Pages = {44-60},
   Publisher = {Elsevier BV},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.07.010},
   Abstract = {The results of a search for pair production of the lighter
             scalar partners of top quarks (t~1) in 2.05 fb-1 of pp
             collisions at s=7 TeV using the ATLAS experiment at the LHC
             are reported. Scalar top quarks are searched for in events
             with two same flavour opposite-sign leptons (e, μ) with
             invariant mass consistent with the Z boson mass, large
             missing transverse momentum and jets in the final state. At
             least one of the jets is identified as originating from a
             b-quark. No excess over Standard Model expectations is
             found. The results are interpreted in the framework of
             R-parity conserving, gauge mediated Supersymmetry breaking
             'natural' scenarios, where the neutralino (χ~10) is the
             next-to-lightest supersymmetric particle. Scalar top quark
             masses up to 310 GeV are excluded for 115GeV&lt;mχ~10&lt;230GeV
             at 95% confidence level, reaching an exclusion of
             mt~1&lt;330GeV for mχ~10=190GeV. Scalar top quark masses
             below 240 GeV are excluded for all values of mχ~10&gt;mZ.
             © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.07.010},
   Key = {fds307791}
}

@article{fds310402,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d’Ascenzo, N and Datta, M and de
             Barbaro, P and Dell’Orso, M and Demortier, L and Deninno, M and Devoto, F and d’Errico, M},
   Title = {Search for scalar top quark production in (Formula
             presented.) collisions at (Formula presented.) = 1.96
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2012)158},
   Abstract = {We report on a search for the supersymmetric partner of the
             top quark (scalar top) decaying into a charm quark and a
             neutralino in (Formula presented.) collisions at (Formula
             presented.) = 1.96TeV. The data sample, collected by the CDF
             II detector at the Fermilab Tevatron, corresponds to an
             integrated luminosity of 2.6 fb<sup>−1</sup>. Candidate
             events are selected by requiring two or more jets and a
             large imbalance in the transverse momentum. To enhance the
             analysis sensitivity, at least one of the jets is required
             to be identified as originating from a charm quark using an
             algorithm specifically designed for this analysis. The
             selected events are in good agreement with standard model
             predictions. In the case of large mass splitting between the
             scalar top quark and the neutralino we exclude a scalar top
             quark mass below 180 GeV/c<sup>2</sup> at 95% confidence
             level.},
   Doi = {10.1007/JHEP10(2012)158},
   Key = {fds310402}
}

@article{fds308218,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon,
             R and Briskin, G and Brock, R and Bross, A and Buchholz, D and Burtovoi,
             VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
             M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
             HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros, Y and Dudko,
             LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
             VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
             OV and Evans, H and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher,
             S and Fein, D and Ferbel, T and Fisk, HE and Fisyak,
             Y},
   Title = {Search for second generation leptoquark pairs decaying to
             μv + jets in pp collisons at √ s = 1.8
             Tev},
   Journal = {Physical Review Letters},
   Volume = {83},
   Number = {15},
   Pages = {2896-2901},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.83.2896},
   Abstract = {We report on a search for second generation leptoquarks (LQ)
             produced in pp collisions at √ = 1.8TeV using the D0
             detector at Fermilab. Second generation leptoquarks are
             assumed to be produced in pairs and to decay to either μ or
             v and either a strange or a charm quark (q). Limits are
             placed on σ (pp → LQLQ → μ v + jets) as a function of
             the mass of the leptoquark. For equal branching ratios to
             μq and vq second generation scalar leptoquarks with a mass
             below 160 GeV/c2 vector leptoquarks with anomalous minimal
             vector couplings with a mass below 240 GeV/c2 and vector
             leptoquarks with Yang-Mills couplings with a mass below 290
             GeV/c2 are excluded at the 95% confidence level. © 1999 The
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.83.2896},
   Key = {fds308218}
}

@article{fds307781,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Search for second generation scalar leptoquarks in pp
             collisions at √s = 7 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {9},
   Pages = {1-21},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2151-6},
   Abstract = {The results of a search for the production of second
             generation scalar leptoquarks are presented for final states
             consisting of either two muons and at least two jets or a
             muon plus missing transverse momentum and at least two jets.
             A total of 1.03 fb<sup>−1</sup> integrated luminosity of
             protonproton collision data produced by the Large Hadron
             Collider at √s = 7 TeV and recorded by the ATLAS detector
             is used for the search. The event yields in the signal
             regions are found to be consistent with the Standard Model
             background expectations. The production of second generation
             leptoquarks is excluded for a leptoquark mass m<inf>LQ</inf>
             < 594 (685) GeV at 95 % confidence level, for a branching
             ratio of 0.5 (1.0) for leptoquark decay to a muon and a
             quark.},
   Doi = {10.1140/epjc/s10052-012-2151-6},
   Key = {fds307781}
}

@article{fds332358,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson,
             EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Burtovoi,
             VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
             K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
             SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
             Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison,
             J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
             T and Fatyga, MK and Feher, S and Fein, D and Ferbel,
             T},
   Title = {Search for second-generation leptoquark pairs in ¯pp
             collisions at √s=1.8TeV},
   Journal = {Physical Review Letters},
   Volume = {84},
   Number = {10},
   Pages = {2088-2093},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.84.2088},
   Abstract = {We have searched for second-generation leptoquark (LQ) pairs
             in the μμ+jets channel using 94 ±5pb−1 of ¯pp collider
             data collected by the D0 experiment at the Fermilab Tevatron
             during 1993–1996. No evidence for a signal is observed.
             These results are combined with those from the μν+jets and
             νν+jets channels to obtain 95% confidence level (C.L.)
             upper limits on the LQ pair production cross section as a
             function of mass and β, the branching fraction of a LQ
             decay into a charged lepton and a quark. Lower limits of
             200(180)GeV/c2 for β=1(1/2) are set at the 95% C.L. on the
             mass of scalar LQ. Mass limits are also set on vector
             leptoquarks as a function of β. © 2000 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.84.2088},
   Key = {fds332358}
}

@article{fds308150,
   Author = {Abulencia, and A, and others},
   Title = {Search for second-generation scalar leptoquarks in
             $p\bar{p}$ collisions at $\sqrt{s} =$ 1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D73},
   Number = {5},
   Pages = {051102},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.72.051107},
   Abstract = {Results on a search for pair production of second generation
             scalar leptoquark in p anti-p collisions at s**(1/2) = 1.96
             TeV are reported. The data analyzed were collected by the
             CDF detector during the 2002-2003 Tevatron Run II and
             correspond to an integrated luminosity of 198 pb-1.
             Leptoquarks (LQ) are sought through their decay into
             (charged) leptons and quarks, with final state signatures
             represented by two muons and jets and one muon, large
             transverse missing energy and jets. We observe no evidence
             for LQ production and derive 95% C.L. upper limits on the LQ
             production cross sections as well as lower limits on their
             mass as a function of Beta, where Beta is the branching
             fraction for LQ --> mu q.},
   Doi = {10.1103/PhysRevD.72.051107},
   Key = {fds308150}
}

@article{fds356789,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Ochoa, MI and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {Search for single b-quark production with the
             ATLAS detector at √s=7 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {721},
   Number = {4-5},
   Pages = {171-189},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.03.016},
   Abstract = {The results of a search for an excited bottom-quark b⁎ in
             pp collisions at s=7 TeV, using 4.7 fb−1 of data collected
             by the ATLAS detector at the LHC are presented. In the model
             studied, a single b⁎-quark is produced through a
             chromomagnetic interaction and subsequently decays to a W
             boson and a top quark. The search is performed in the
             dilepton and lepton + jets final states, which are combined
             to set limits on b⁎-quark couplings for a range of
             b⁎-quark masses. For a benchmark with unit size
             chromomagnetic and Standard Model-like electroweak b⁎
             couplings, b⁎ quarks with masses less than 870 GeV are
             excluded at the 95% credibility level.},
   Doi = {10.1016/j.physletb.2013.03.016},
   Key = {fds356789}
}

@article{fds315924,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O},
   Title = {Search for single production of a vector-like quark via a
             heavy gluon in the 4b final state with the ATLAS detector in
             pp collisions at s=8 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {758},
   Pages = {249-268},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {July},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.04.061},
   Abstract = {A search is performed for the process pp→G*→BHb-/B-Hb→Hbb-→bb-bb-,
             predicted in composite Higgs scenarios, where G* is a heavy
             colour octet vector resonance and BH a vector-like quark of
             charge -1/3. The data were obtained from pp collisions at a
             centre-of-mass energy of 8 TeV corresponding to an
             integrated luminosity of 19.5 fb-1, recorded by the ATLAS
             detector at the LHC. The largest background, multijet
             production, is estimated using a data-driven method. No
             significant excess of events with respect to Standard Model
             predictions is observed, and upper limits on the production
             cross section times branching ratio are set. Comparisons to
             the predictions from a specific benchmark model are made,
             resulting in lower mass limits in the two-dimensional mass
             plane of mG* vs. mBH.},
   Doi = {10.1016/j.physletb.2016.04.061},
   Key = {fds315924}
}

@article{fds321106,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako,
             K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro,
             LB and Barreiro, F and Costa, JBGD and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov,
             VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella,
             G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
             JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford,
             L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and de
             Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
             G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
             T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich,
             LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
             DG and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella,
             G},
   Title = {Search for single production of vector-like quarks decaying
             into Wb in pp collisions at [Formula: see
             text] TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {8},
   Pages = {442},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4281-8},
   Abstract = {A search for singly produced vector-like <i>Q</i> quarks,
             where <i>Q</i> can be either a <i>T</i> quark with charge
             [Formula: see text] or a <i>Y</i> quark with charge
             [Formula: see text], is performed in proton-proton
             collisions recorded with the ATLAS detector at the LHC. The
             dataset corresponds to an integrated luminosity of 20.3
             fb[Formula: see text] and was produced with a centre-of-mass
             energy of [Formula: see text] TeV. This analysis targets
             [Formula: see text] decays where the <i>W</i> boson decays
             leptonically. A veto on massive large-radius jets is used to
             reject the dominant [Formula: see text] background. The
             reconstructed <i>Q</i>-candidate mass, ranging from 0.4 to
             1.2 TeV, is used in the search to discriminate signal from
             background processes. No significant deviation from the
             Standard Model expectation is observed, and limits are set
             on the [Formula: see text] cross-section times branching
             ratio. The results are also interpreted as limits on the
             <i>QWb</i> coupling and the mixing with the Standard Model
             sector for a singlet <i>T</i> quark or a <i>Y</i> quark from
             a doublet. <i>T</i> quarks with masses below 0.95 TeV are
             excluded at 95 % confidence level, assuming a unit coupling
             and a BR[Formula: see text], whereas the expected limit is
             1.10 TeV.},
   Doi = {10.1140/epjc/s10052-016-4281-8},
   Key = {fds321106}
}

@article{fds356605,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {Search for single production of vector-like quarks decaying
             into Wb in pp collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {5},
   Year = {2019},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2019)164},
   Abstract = {A search for singly produced vector-like quarks Q, where Q
             can be either a T quark with charge +2/3 or a Y quark with
             charge −4/3, is performed in proton–proton collision
             data at a centre-of-mass energy of 13 TeV corresponding to
             an integrated luminosity of 36.1 fb−1, recorded with the
             ATLAS detector at the LHC in 2015 and 2016. The analysis
             targets Q → Wb decays where the W boson decays
             leptonically. No significant deviation from the expected
             Standard Model background is observed. Upper limits are set
             on the QWb coupling strength and the mixing between the
             Standard Model sector and a singlet T quark or a Y quark
             from a (B, Y) doublet or a (T, B, Y) triplet, taking into
             account the interference effects with the Standard Model
             background. The upper limits set on the mixing angle are as
             small as |sin θL| = 0.18 for a singlet T quark of mass 800
             GeV, |sin θR| = 0.17 for a Y quark of mass 800 GeV in a (B,
             Y) doublet model and |sin θL| = 0.16 for a Y quark of mass
             800 GeV in a (T, B, Y) triplet model. Within a (B, Y)
             doublet model, the limits set on the mixing parameter |sin
             θR| are comparable with the exclusion limits from
             electroweak precision observables in the mass range between
             about 900 GeV and 1250 GeV.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP05(2019)164},
   Key = {fds356605}
}

@article{fds308185,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin,
             B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto,
             J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Boos, EE and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler,
             JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del
             Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and di Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing,
             S},
   Title = {Search for single top quark production at DØ using neural
             networks},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {517},
   Number = {3-4},
   Pages = {282-294},
   Publisher = {Elsevier BV},
   Year = {2001},
   Month = {October},
   url = {http://dx.doi.org/10.1016/S0370-2693(01)01009-7},
   Abstract = {We present a search for electroweak production of single top
             quarks in ≈90 pb-1 of data collected with the DØ detector
             at the Fermilab Tevatron collider. Using arrays of neural
             networks to separate signals from backgrounds, we set upper
             limits on the cross sections of 17 pb for the s-channel
             process pp̄ → tb + X, and 22 pb for the t-channel process
             pp̄ → tqb + X, both at the 95% confidence level. © 2001
             Elsevier Science B.V. All rights reserved.},
   Doi = {10.1016/S0370-2693(01)01009-7},
   Key = {fds308185}
}

@article{fds307918,
   Author = {Aaltonen, and T, and others},
   Title = {Search for single top quark production in $\bar{p} p$
             collisions at $\sqrt{s} = 1.96$ TeV in the missing
             transverse energy plus jets topology},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {7},
   Pages = {072003},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.072003},
   Abstract = {http://arxiv.org/abs/1001.4577},
   Doi = {10.1103/PhysRevD.81.072003},
   Key = {fds307918}
}

@article{fds308222,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Alves, GA and Amos, N and Anderson,
             EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov,
             VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland,
             T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {Search for squarks and gluinos in events containing jets and
             a large imbalance in transverse energy},
   Journal = {Physical Review Letters},
   Volume = {83},
   Number = {24},
   Pages = {4937-4942},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.83.4937},
   Abstract = {Using data corresponding to an integrated luminosity of
             79pb−1, D0 has searched for events containing multiple
             jets and large missing transverse energy in pp¯ collisions
             at √s = 1.8TeV at the Fermilab Tevatron collider.
             Observing no significant excess beyond what is expected from
             the standard model, we set limits on the masses of squarks
             and gluinos and on the model parameters m0 and m1/2, in the
             framework of the minimal low-energy supergravity models of
             supersymmetry. For tanβ=2 and A0 = 0, with μ < 0, we
             exclude all models with m˜q<250 GeV/c2. For models with
             equal squark and gluino masses, we exclude m < 260 GeV/c2.
             © 1999 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.83.4937},
   Key = {fds308222}
}

@article{fds356720,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
             LJ},
   Title = {Search for squarks and gluinos in events with an isolated
             lepton, jets, and missing transverse momentum at √s=13 TeV
             with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {96},
   Number = {11},
   Year = {2017},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.96.112010},
   Abstract = {The results of a search for squarks and gluinos in final
             states with an isolated electron or muon, multiple jets and
             large missing transverse momentum using proton-proton
             collision data at a center-of-mass energy of √ = 13 TeV
             are presented. The data set used was recorded during 2015
             and 2016 by the ATLAS experiment at the Large Hadron
             Collider and corresponds to an integrated luminosity of 36.1
             fb-1. No significant excess beyond the expected background
             is found. Exclusion limits at 95% confidence level are set
             in a number of supersymmetric scenarios, reaching masses up
             to 2.1 TeV for gluino pair production and up to 1.25 TeV for
             squark pair production.},
   Doi = {10.1103/PhysRevD.96.112010},
   Key = {fds356720}
}

@article{fds346229,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
             YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
             S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier,
             S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M},
   Title = {Search for squarks and gluinos in events with hadronically
             decaying tau leptons, jets and missing transverse momentum
             in proton-proton collisions at [Formula: see text] TeV
             recorded with the ATLAS detector.},
   Journal = {Eur Phys J C Part Fields},
   Volume = {76},
   Number = {12},
   Pages = {683},
   Year = {2016},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4481-2},
   Abstract = {A search for supersymmetry in events with large missing
             transverse momentum, jets, and at least one hadronically
             decaying tau lepton has been performed using
             3.2 fb[Formula: see text] of proton-proton collision data
             at [Formula: see text] recorded by the ATLAS detector at the
             Large Hadron Collider in 2015. Two exclusive final states
             are considered, with either exactly one or at least two tau
             leptons. No excess over the Standard Model prediction is
             observed in the data. Results are interpreted in the context
             of gauge-mediated supersymmetry breaking and a simplified
             model of gluino pair production with tau-rich cascade
             decays, substantially improving on previous limits. In the
             GMSB model considered, supersymmetry-breaking scale
             ([Formula: see text]) values below [Formula: see text] are
             excluded at the 95% confidence level, corresponding to
             gluino masses below [Formula: see text]. For large values of
             [Formula: see text], values of [Formula: see text] up to
             [Formula: see text] and gluino masses up to [Formula: see
             text] are excluded. In the simplified model, gluino masses
             are excluded up to [Formula: see text] for neutralino masses
             around [Formula: see text]. Neutralino masses below
             [Formula: see text] are excluded for all gluino masses
             between 800 and [Formula: see text], while the strongest
             exclusion of [Formula: see text] is achieved for gluino
             masses around [Formula: see text].},
   Doi = {10.1140/epjc/s10052-016-4481-2},
   Key = {fds346229}
}

@article{fds310292,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
             M},
   Title = {Search for squarks and gluinos in events with isolated
             leptons, jets and missing transverse momentum at √s = 8
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {4},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2015)116},
   Abstract = {The results of a search for supersymmetry in final states
             containing at least one isolated lepton (electron or muon),
             jets and large missing transverse momentum with the ATLAS
             detector at the Large Hadron Collider are reported. The
             search is based on proton-proton collision data at a
             centre-of-mass energy √ = 8 TeV collected in 2012,
             corresponding to an integrated luminosity of 20 fb−1. No
             significant excess above the Standard Model expectation is
             observed. Limits are set on supersymmetric particle masses
             for various supersymmetric models. Depending on the model,
             the search excludes gluino masses up to 1.32 TeV and squark
             masses up to 840 GeV. Limits are also set on the parameters
             of a minimal universal extra dimension model, excluding a
             compactification radius of 1/Rc = 950 GeV for a cut-off
             scale times radius (ΛRc) of approximately
             30.},
   Doi = {10.1007/JHEP04(2015)116},
   Key = {fds310292}
}

@article{fds347452,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
   Title = {Search for squarks and gluinos in final states with
             hadronically decaying τ -leptons, jets, and missing
             transverse momentum using pp collisions at s =13 TeV with
             the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {99},
   Number = {1},
   Year = {2019},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.99.012009},
   Abstract = {A search for supersymmetry in events with large missing
             transverse momentum, jets, and at least one hadronically
             decaying τ-lepton is presented. Two exclusive final states
             with either exactly one or at least two τ-leptons are
             considered. The analysis is based on proton-proton
             collisions at s=13 TeV corresponding to an integrated
             luminosity of 36.1 fb-1 delivered by the Large Hadron
             Collider and recorded by the ATLAS detector in 2015 and
             2016. No significant excess is observed over the Standard
             Model expectation. At 95% confidence level,
             model-independent upper limits on the cross section are set
             and exclusion limits are provided for two signal scenarios:
             a simplified model of gluino pair production with τ-rich
             cascade decays, and a model with gauge-mediated
             supersymmetry breaking (GMSB). In the simplified model,
             gluino masses up to 2000 GeV are excluded for low values of
             the mass of the lightest supersymmetric particle (LSP),
             while LSP masses up to 1000 GeV are excluded for gluino
             masses around 1400 GeV. In the GMSB model, values of the
             supersymmetry-breaking scale are excluded below 110 TeV for
             all values of tanβ in the range 2≤tanβ≤60, and below
             120 TeV for tanβ>30.},
   Doi = {10.1103/PhysRevD.99.012009},
   Key = {fds347452}
}

@article{fds321117,
   Author = {Atlas Collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
             Kuutmann, E and Berger, N and Beringer, J and Berlendis, S and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
             De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro,
             R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero,
             J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
             Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
   Title = {Search for squarks and gluinos in final states with jets and
             missing transverse momentum at [Formula: see text] =13
             [Formula: see text]with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {7},
   Pages = {392},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4184-8},
   Abstract = {A search for squarks and gluinos in final states containing
             hadronic jets, missing transverse momentum but no electrons
             or muons is presented. The data were recorded in 2015 by the
             ATLAS experiment in [Formula: see text] proton-proton
             collisions at the Large Hadron Collider. No excess above the
             Standard Model background expectation was observed in
             3.2 [Formula: see text] of analyzed data. Results are
             interpreted within simplified models that assume
             <i>R</i>-parity is conserved and the neutralino is the
             lightest supersymmetric particle. An exclusion limit at the
             95 % confidence level on the mass of the gluino is set at
             1.51 [Formula: see text] for a simplified model
             incorporating only a gluino octet and the lightest
             neutralino, assuming the lightest neutralino is massless.
             For a simplified model involving the strong production of
             mass-degenerate first- and second-generation squarks, squark
             masses below 1.03 [Formula: see text] are excluded for a
             massless lightest neutralino. These limits substantially
             extend the region of supersymmetric parameter space excluded
             by previous measurements with the ATLAS detector.},
   Doi = {10.1140/epjc/s10052-016-4184-8},
   Key = {fds321117}
}

@article{fds355441,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
             C},
   Title = {Search for squarks and gluinos in final states with jets and
             missing transverse momentum using 139 fb −1 of
             √s = 13 TeV pp collision data with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {2},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP02(2021)143},
   Abstract = {A search for the supersymmetric partners of quarks and
             gluons (squarks and gluinos) in final states containing jets
             and missing transverse momentum, but no electrons or muons,
             is presented. The data used in this search were recorded by
             the ATLAS experiment in proton-proton collisions at a
             centre-of-mass energy of s = 13 TeV during Run 2 of the
             Large Hadron Collider, corresponding to an integrated
             luminosity of 139 fb−1. The results are interpreted in the
             context of various R-parity-conserving models where squarks
             and gluinos are produced in pairs or in association and a
             neutralino is the lightest supersymmetric particle. An
             exclusion limit at the 95% confidence level on the mass of
             the gluino is set at 2.30 TeV for a simplified model
             containing only a gluino and the lightest neutralino,
             assuming the latter is massless. For a simplified model
             involving the strong production of mass-degenerate first-
             and second-generation squarks, squark masses below 1.85 TeV
             are excluded if the lightest neutralino is massless. These
             limits extend substantially beyond the region of
             supersymmetric parameter space excluded previously by
             similar searches with the ATLAS detector. [Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP02(2021)143},
   Key = {fds355441}
}

@article{fds356680,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
             LJ},
   Title = {Search for squarks and gluinos in final states with jets and
             missing transverse momentum using 36 fb-1 of √s =13 TeV pp
             collision data with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {97},
   Number = {11},
   Year = {2018},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.97.112001},
   Abstract = {A search for the supersymmetric partners of quarks and
             gluons (squarks and gluinos) in final states containing
             hadronic jets and missing transverse momentum, but no
             electrons or muons, is presented. The data used in this
             search were recorded in 2015 and 2016 by the ATLAS
             experiment in s=13 TeV proton-proton collisions at the Large
             Hadron Collider, corresponding to an integrated luminosity
             of 36.1 fb-1. The results are interpreted in the context of
             various models where squarks and gluinos are pair produced
             and the neutralino is the lightest supersymmetric particle.
             An exclusion limit at the 95% confidence level on the mass
             of the gluino is set at 2.03 TeV for a simplified model
             incorporating only a gluino and the lightest neutralino,
             assuming the lightest neutralino is massless. For a
             simplified model involving the strong production of
             mass-degenerate first- and second-generation squarks, squark
             masses below 1.55 TeV are excluded if the lightest
             neutralino is massless. These limits substantially extend
             the region of supersymmetric parameter space previously
             excluded by searches with the ATLAS detector.},
   Doi = {10.1103/PhysRevD.97.112001},
   Key = {fds356680}
}

@article{fds366275,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
             C},
   Title = {Search for squarks and gluinos in final states with one
             isolated lepton, jets, and missing transverse momentum at
             √s=13 with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {7},
   Year = {2021},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09344-w},
   Abstract = {The results of a search for gluino and squark pair
             production with the pairs decaying via the lightest
             charginos into a final state consisting of two W bosons, the
             lightest neutralinos (χ~10), and quarks, are presented: the
             signal is characterised by the presence of a single charged
             lepton (e± or μ±) from a W boson decay, jets, and missing
             transverse momentum. The analysis is performed using
             139 fb- 1 of proton–proton collision data taken at a
             centre-of-mass energy s=13 delivered by the Large Hadron
             Collider and recorded by the ATLAS experiment. No
             statistically significant excess of events above the
             Standard Model expectation is found. Limits are set on the
             direct production of squarks and gluinos in simplified
             models. Masses of gluino (squark) up to 2.2 (1.4) are
             excluded at 95% confidence level for a light
             χ~10.},
   Doi = {10.1140/epjc/s10052-021-09344-w},
   Key = {fds366275}
}

@article{fds350334,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
             Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V},
   Title = {Search for squarks and gluinos in final states with
             same-sign leptons and jets using 139 fb −1 of
             data collected with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {6},
   Year = {2020},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2020)046},
   Abstract = {A search for supersymmetric partners of gluons and quarks is
             presented, involving signatures with jets and either two
             isolated leptons (electrons or muons) with the same electric
             charge, or at least three isolated leptons. A data sample of
             proton-proton collisions at s = 13 TeV recorded with the
             ATLAS detector at the Large Hadron Collider between 2015 and
             2018, corresponding to a total integrated luminosity of 139
             fb−1, is used for the search. No significant excess over
             the Standard Model expectation is observed. The results are
             interpreted in simplified supersymmetric models featuring
             both R-parity conservation and R-parity violation, raising
             the exclusion limits beyond those of previous ATLAS searches
             to 1600 GeV for gluino masses and 750 GeV for bottom and top
             squark masses in these scenarios. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP06(2020)046},
   Key = {fds350334}
}

@article{fds308212,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Balamurali, V and Baldin, B and Banerjee,
             S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding,
             F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey,
             D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang,
             SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger,
             C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
             P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
             G},
   Title = {Search for squarks and gluinos in single-photon events with
             jets and large missing transverse energy in p¯p collisions
             at √ s = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {82},
   Number = {1},
   Pages = {29-34},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.82.29},
   Abstract = {We search for new physics using events with one high
             transverse energy photon, two or more jets, and an apparent
             imbalance in transverse energy, in pp¯ collisions at the
             Fermilab Tevatron at √ s=1.8TeV. Such events are predicted
             for production of supersymmetric particles in some models.
             No excess is observed beyond expected background. For the
             parameter space of the minimal supersymmetric standard model
             with branching fraction B(∼ Χ02→ = γ ∼ Χ01) = 1 and
             mΧ02- mΧ01> 20 GeV, we obtain a 95% confidence level lower
             mass limit of 310 GeV for equal mass squarks and gluinos.
             The results are also interpreted in models with low energy
             gauge mediated supersymmetry breaking. © 1999 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.82.29},
   Key = {fds308212}
}

@article{fds307755,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for squarks and gluinos using final states with jets
             and missing transverse momentum with the Atlas detector in
             s=7 TeV proton-proton collisions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {710},
   Number = {1},
   Pages = {67-85},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.051},
   Abstract = {A search for squarks and gluinos in events containing jets,
             missing transverse momentum and no electrons or muons is
             presented. The data were recorded in 2011 by the ATLAS
             experiment in s=7 TeV proton-proton collisions at the Large
             Hadron Collider. No excess above the Standard Model
             background expectation is observed in 1.04 fb-1 of data.
             Gluino and squark masses below 700 GeV and 875 GeV
             respectively are excluded at the 95% confidence level in
             simplified models containing only squarks of the first two
             generations, a gluino octet and a massless neutralino. The
             exclusion limit increases to 1075 GeV for squarks and
             gluinos of equal mass. In MSUGRA/CMSSM models with tanβ=10,
             A0=0 and μ>0, squarks and gluinos of equal mass are
             excluded for masses below 950 GeV. These limits extend the
             region of supersymmetric parameter space excluded by
             previous measurements. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.02.051},
   Key = {fds307755}
}

@article{fds307633,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Search for squarks and gluinos with the ATLAS detector in
             final states with jets and missing transverse momentum using
             4.7 fb-1 of √s=7 TeV proton-proton collision
             data},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.012008},
   Abstract = {A search for squarks and gluinos in final states containing
             jets, missing transverse momentum and no high-pT electrons
             or muons is presented. The data represent the complete
             sample recorded in 2011 by the ATLAS experiment in 7 TeV
             proton-proton collisions at the Large Hadron Collider, with
             a total integrated luminosity of 4.7 fb-1. No excess above
             the Standard Model background expectation is observed.
             Gluino masses below 860 GeV and squark masses below 1320 GeV
             are excluded at the 95% confidence level in simplified
             models containing only squarks of the first two generations,
             a gluino octet and a massless neutralino, for squark or
             gluino masses below 2 TeV, respectively. Squarks and gluinos
             with equal masses below 1410 GeV are excluded. In minimal
             supergravity/constrained minimal supersymmetric Standard
             Model models with tanâ-¡β=10, A0=0 and μ>0, squarks and
             gluinos of equal mass are excluded for masses below 1360
             GeV. Constraints are also placed on the parameter space of
             supersymmetric models with compressed spectra. These limits
             considerably extend the region of supersymmetric parameter
             space excluded by previous measurements with the ATLAS
             detector.},
   Doi = {10.1103/PhysRevD.87.012008},
   Key = {fds307633}
}

@article{fds310367,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for squarks and gluinos with the ATLAS detector in
             final states with jets and missing transverse momentum using
             √s = 8 TeV proton-proton collision data},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2014)176},
   Abstract = {A search for squarks and gluinos in final states containing
             high-pTjets, missing transverse momentum and no electrons or
             muons is presented. The data were recorded in 2012 by the
             ATLAS experiment in √s = 8TeV proton-proton collisions at
             the Large Hadron Collider, with a total integrated
             luminosity of 20.3 fb−1. Results are interpreted in a
             variety of simplified and specific supersymmetry-breaking
             models assuming that R-parity is conserved and that the
             lightest neutralino is the lightest supersymmetric particle.
             An exclusion limit at the 95% confidence level on the mass
             of the gluino is set at 1330GeV for a simplified model
             incorporating only a gluino and the lightest neutralino. For
             a simplified model involving the strong production of first-
             and second-generation squarks, squark masses below 850GeV
             (440GeV) are excluded for a massless lightest neutralino,
             assuming mass degenerate (single light-flavour) squarks. In
             mSUGRA/CMSSM models with tan β = 30, A0= −2m0and μ > 0,
             squarks and gluinos of equal mass are excluded for masses
             below 1700GeV. Additional limits are set for non-universal
             Higgs mass models with gaugino mediation and for simplified
             models involving the pair production of gluinos, each
             decaying to a top squark and a top quark, with the top
             squark decaying to a charm quark and a neutralino. These
             limits extend the region of supersymmetric parameter space
             excluded by previous searches with the ATLAS
             detector.},
   Doi = {10.1007/JHEP09(2014)176},
   Key = {fds310367}
}

@article{fds313575,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
             F and Bednar, P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
             A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
             A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli,
             M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi,
             R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G},
   Title = {Search for standard model Higgs boson production in
             association with a W boson at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {78},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   Month = {August},
   ISSN = {1550-7998},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000258975300012&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Abstract = {We present a search for standard model Higgs boson
             production in association with a W boson in
             proton-antiproton collisions (pp̄→ W±H→ νbb̄) at a
             center of mass energy of 1.96 TeV. The search employs data
             collected with the CDF II detector which correspond to an
             integrated luminosity of approximately 1fb-1. We select
             events consistent with a signature of a single lepton
             (e±/μ±), missing transverse energy, and two jets. Jets
             corresponding to bottom quarks are identified with a
             secondary vertex tagging method and a neural network filter
             technique. The observed number of events and the dijet mass
             distributions are consistent with the standard model
             background expectations, and we set 95% confidence level
             upper limits on the production cross section times branching
             ratio ranging from 3.9 to 1.3 pb for Higgs boson masses from
             110 to 150GeV/c2, respectively. © 2008 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.78.032008},
   Key = {fds313575}
}

@article{fds307808,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci,
             MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F},
   Title = {Search for standard model Higgs boson production in
             association with a W boson using a matrix element technique
             at CDF in pp̄ collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.072001},
   Abstract = {This paper presents a search for standard model Higgs boson
             production in association with a W boson using events
             recorded by the CDF experiment in a data set corresponding
             to an integrated luminosity of 5.6fb -1. The search is
             performed using a matrix element technique in which the
             signal and background hypotheses are used to create a
             powerful discriminator. The discriminant output
             distributions for signal and background are fit to the
             observed events using a binned likelihood approach to search
             for the Higgs boson signal. We find no evidence for a Higgs
             boson, and 95% confidence level (C.L.) upper limits are set
             on σ(pp̄→WH)×B(H→bb̄). The observed limits range
             from 3.5 to 37.6 relative to the standard model expectation
             for Higgs boson masses between m H=100GeV/c2 and m
             H=150GeV/c2. The 95% C.L. expected limit is estimated from
             the median of an ensemble of simulated experiments and
             varies between 2.9 and 32.7 relative to the production rate
             predicted by the standard model over the Higgs boson mass
             range studied. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.85.072001},
   Key = {fds307808}
}

@article{fds307997,
   Author = {Aaltonen, T and others},
   Title = {Search for standard model Higgs boson production in
             association with a W boson using a neural network
             discriminant at CDF},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {1},
   Pages = {012002},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.012002},
   Abstract = {We present a search for standard model Higgs boson
             production in association with a W boson in
             proton-antiproton collisions (pp̅ →W &plusmn;
             H→ℓνbb̅ ) at a center of mass energy of 1.96 TeV. The
             search employs data collected with the CDF II detector that
             correspond to an integrated luminosity of approximately
             1.9  fb-1. We select events consistent with a signature
             of a single charged lepton (e &plusmn; /μ &plusmn; ),
             missing transverse energy, and two jets. Jets corresponding
             to bottom quarks are identified with a secondary vertex
             tagging method, a jet probability tagging method, and a
             neural network filter. We use kinematic information in an
             artificial neural network to improve discrimination between
             signal and background compared to previous analyses. The
             observed number of events and the neural network output
             distributions are consistent with the standard model
             background expectations, and we set 95% confidence level
             upper limits on the production cross section times branching
             fraction ranging from 1.2 to 1.1 pb or 7.5 to 102 times the
             standard model expectation for Higgs boson masses from 110
             to 150  GeV/c2, respectively.},
   Doi = {10.1103/PhysRevD.80.012002},
   Key = {fds307997}
}

@article{fds356656,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Search for standard-model Z and Higgs bosons decaying into a
             bottom-antibottom quark pair in proton-antiproton collisions
             at 1.96 TeV SEARCH for STANDARD-MODEL Z and HIGGS ... T.
             AALTONEN et al.},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {7},
   Year = {2018},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.072002},
   Abstract = {The Collider Detector at Fermilab collected a unique sample
             of jets originating from bottom-quark fragmentation (b-jets)
             by selecting online proton-antiproton (pp̄) collisions with
             a vertex displaced from the pp̄ interaction point,
             consistent with the decay of a bottom-quark hadron. This
             data set, collected at a center-of-mass energy of 1.96 TeV,
             and corresponding to an integrated luminosity of 5.4 fb-1,
             is used to measure the Z-boson production cross section
             times branching ratio into bb̄. The number of Z→bb̄
             events is determined by fitting the dijet-mass distribution,
             while constraining the dominant b-jet background,
             originating from QCD multijet events, with data. The result,
             σ(pp̄→Z)×B(Z→bb̄)=1.11±0.08(stat)±0.14(syst) nb,
             is the most precise measurement of this process, and is
             consistent with the standard-model prediction. The data set
             is also used to search for Higgs-boson production. No
             significant signal is expected in our data and the first
             upper limit on the cross section for the inclusive
             pp̄→H→bb̄ process at s=1.96 TeV is set, corresponding
             to 33 times the expected standard-model cross section, or
             σ=40.6 pb, at the 95% confidence level.},
   Doi = {10.1103/PhysRevD.98.072002},
   Key = {fds356656}
}

@article{fds356777,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Search for strong gravity in multijet final states produced
             in pp collisions at √s = 13 TeV using the ATLAS detector
             at the LHC},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {3},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2016)026},
   Abstract = {Abstract: A search is conducted for new physics in multijet
             final states using 3.6 inverse femtobarns of data from
             proton-proton collisions at (Formula presented.) TeV taken
             at the CERN Large Hadron Collider with the ATLAS detector.
             Events are selected containing at least three jets with
             scalar sum of jet transverse momenta (HT) greater than 1
             TeV. No excess is seen at large HTand limits are presented
             on new physics: models which produce final states containing
             at least three jets and having cross sections larger than
             1.6 fb with HT> 5.8 TeV are excluded. Limits are also given
             in terms of new physics models of strong gravity that
             hypothesize additional space-time dimensions.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP03(2016)026},
   Key = {fds356777}
}

@article{fds307767,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni,
             G and Arutinov, D},
   Title = {Search for strong gravity signatures in same-sign dimuon
             final states using the ATLAS detector at the
             LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {709},
   Number = {4-5},
   Pages = {322-340},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.049},
   Abstract = {A search for microscopic black holes has been performed in a
             same-sign dimuon final state using 1.3 fb -1 of
             proton-proton collision data collected with the ATLAS
             detector at a centre of mass energy of 7 TeV at the CERN
             Large Hadron Collider. The data are found to be consistent
             with the expectation from the Standard Model and the results
             are used to derive exclusion contours in the context of a
             low scale gravity model. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.02.049},
   Key = {fds307767}
}

@article{fds313589,
   Author = {The, ATLASC and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek,
             S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J},
   Title = {Search for strong production of supersymmetric particles in
             final states with missing transverse momentum and at least
             three b-jets at (formula presented) TeV proton-proton
             collisions with the ATLAS detector},
   Journal = {Critical Ultrasound Journal},
   Volume = {2014},
   Number = {10},
   Year = {2014},
   Month = {January},
   ISSN = {1126-6708},
   url = {http://dx.doi.org/10.1007/JHEP10(2014)024},
   Abstract = {© 2014, The Author(s). Abstract: This paper reports the
             results of a search for strong production of supersymmetric
             particles in 20.1 fb−1 of proton-proton collisions at a
             centre-of-mass energy of 8 TeV using the ATLAS detector at
             the LHC. The search is performed separately in events with
             either zero or at least one high-pT lepton (electron or
             muon), large missing transverse momentum, high jet
             multiplicity and at least three jets identified as
             originated from the fragmentation of a b-quark. No excess is
             observed with respect to the Standard Model predictions. The
             results are interpreted in the context of several
             supersymmetric models involving gluinos and scalar top and
             bottom quarks, as well as a mSUGRA/CMSSM model. Gluino
             masses up to 1340 GeV are excluded, depending on the model,
             significantly extending the previous ATLAS
             limits.},
   Doi = {10.1007/JHEP10(2014)024},
   Key = {fds313589}
}

@article{fds315921,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
             K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
             De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
             TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan,
             SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Search for supersymmetry at [Formula: see text] TeV in
             final states with jets and two same-sign leptons or three
             leptons with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {259},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4095-8},
   Abstract = {A search for strongly produced supersymmetric particles is
             conducted using signatures involving multiple energetic jets
             and either two isolated leptons (<i>e</i> or [Formula: see
             text]) with the same electric charge or at least three
             isolated leptons. The search also utilises <i>b</i>-tagged
             jets, missing transverse momentum and other observables to
             extend its sensitivity. The analysis uses a data sample of
             proton-proton collisions at [Formula: see text] TeV
             recorded with the ATLAS detector at the Large Hadron
             Collider in 2015 corresponding to a total integrated
             luminosity of 3.2 fb[Formula: see text]. No significant
             excess over the Standard Model expectation is observed. The
             results are interpreted in several simplified supersymmetric
             models and extend the exclusion limits from previous
             searches. In the context of exclusive production and
             simplified decay modes, gluino masses are excluded at
             [Formula: see text] confidence level up to 1.1-1.3 TeV for
             light neutralinos (depending on the decay channel), and
             bottom squark masses are also excluded up to 540 GeV. In the
             former scenarios, neutralino masses are also excluded up to
             550-850 GeV for gluino masses around 1 TeV.},
   Doi = {10.1140/epjc/s10052-016-4095-8},
   Key = {fds315921}
}

@article{fds310378,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Coutinho, YA and Amelung,
             C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for supersymmetry at √s= 8 TeV in final states with
             jets and two same-sign leptons or three leptons with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP06(2014)035},
   Abstract = {A search for strongly produced supersymmetric particles is
             conducted using signatures involving multiple energetic jets
             and either two isolated leptons (e or μ) with the same
             electric charge, or at least three isolated leptons. The
             search also utilises jets originating from b-quarks, missing
             transverse momentum and other observables to extend its
             sensitivity. The analysis uses a data sample corresponding
             to a total integrated luminosity of 20.3 fb-1 of √s = 8
             TeV proton-proton collisions recorded with the ATLAS
             detector at the Large Hadron Collider in 2012. No deviation
             from the Standard Model expectation is observed. New or
             significantly improved exclusion limits are set on a wide
             variety of supersymmetric models in which the lightest
             squark can be of the first, second or third generations, and
             in which R-parity can be conserved or violated. [Figure not
             available: see fulltext.] © 2014 The Author(s).},
   Doi = {10.1007/JHEP06(2014)035},
   Key = {fds310378}
}

@article{fds321093,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali,
             B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
             YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
             S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier,
             S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M},
   Title = {Search for supersymmetry in a final state containing two
             photons and missing transverse momentum in [Formula: see
             text] = 13 TeV [Formula: see text] collisions at the LHC
             using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {9},
   Pages = {517},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4344-x},
   Abstract = {A search has been made for supersymmetry in a final state
             containing two photons and missing transverse momentum using
             the ATLAS detector at the Large Hadron Collider. The search
             makes use of [Formula: see text] of proton-proton collision
             data collected at a centre-of-mass energy of 13 TeV in
             2015. Using a combination of data-driven and
             Monte-Carlo-based approaches, the Standard Model background
             is estimated to be [Formula: see text] events. No events are
             observed in the signal region; considering the expected
             background and its uncertainty, this observation implies a
             model-independent 95 % CL upper limit of 0.93 fb (3.0
             events) on the visible cross section due to physics beyond
             the Standard Model. In the context of a generalized model of
             gauge-mediated supersymmetry breaking with a bino-like
             next-to-lightest supersymmetric particle, this leads to a
             lower limit of 1650 GeV on the mass of a degenerate octet
             of gluino states, independent of the mass of the lighter
             bino-like neutralino.},
   Doi = {10.1140/epjc/s10052-016-4344-x},
   Key = {fds321093}
}

@article{fds313617,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Piqueras, DÁ and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
             C},
   Title = {Search for supersymmetry in events containing a same-flavour
             opposite-sign dilepton pair, jets, and large missing
             transverse momentum in [Formula: see text] TeV pp
             collisions with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {318},
   Year = {2015},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3518-2},
   Abstract = {Two searches for supersymmetric particles in final states
             containing a same-flavour opposite-sign lepton pair, jets
             and large missing transverse momentum are presented. The
             proton-proton collision data used in these searches were
             collected at a centre-of-mass energy [Formula: see
             text] TeV by the ATLAS detector at the Large Hadron
             Collider and corresponds to an integrated luminosity of
             20.3 fb[Formula: see text]. Two leptonic production
             mechanisms are considered: decays of squarks and gluinos
             with <i>Z</i> bosons in the final state, resulting in a peak
             in the dilepton invariant mass distribution around the
             <i>Z</i>-boson mass; and decays of neutralinos (e.g.
             [Formula: see text]), resulting in a kinematic endpoint in
             the dilepton invariant mass distribution. For the former, an
             excess of events above the expected Standard Model
             background is observed, with a significance of three
             standard deviations. In the latter case, the data are
             well-described by the expected Standard Model background.
             The results from each channel are interpreted in the context
             of several supersymmetric models involving the production of
             squarks and gluinos.},
   Doi = {10.1140/epjc/s10052-015-3518-2},
   Key = {fds313617}
}

@article{fds356728,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Search for supersymmetry in events with b-tagged jets and
             missing transverse momentum in pp collisions at √s=13 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {11},
   Year = {2017},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2017)195},
   Abstract = {A search for the supersymmetric partners of the Standard
             Model bottom and top quarks is presented. The search uses
             36.1 fb−1 of pp collision data at s=13 TeV collected by
             the ATLAS experiment at the Large Hadron Collider. Direct
             production of pairs of bottom and top squarks (b¯ 1 and t¯
             1) is searched for in final states with b-tagged jets and
             missing transverse momentum. Distinctive selections are
             defined with either no charged leptons (electrons or muons)
             in the final state, or one charged lepton. The zero-lepton
             selection targets models in which the b¯ 1 is the lightest
             squark and decays via b¯1→bχ¯10, where χ¯10 is the
             lightest neutralino. The one-lepton final state targets
             models where bottom or top squarks are produced and can
             decay into multiple channels, b¯1→bχ¯10 and b¯1→t or
             t¯1→tχ¯10 and t¯1→b where χ¯1± is the lightest
             chargino and the mass difference mχ¯1±−mχ¯10 is set
             to 1 GeV. No excess above the expected Standard Model
             background is observed. Exclusion limits at 95% confidence
             level on the mass of third-generation squarks are derived in
             various supersymmetry-inspired simplified
             models.},
   Doi = {10.1007/JHEP11(2017)195},
   Key = {fds356728}
}

@article{fds366277,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
             N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
             C},
   Title = {Search for supersymmetry in events with four or more charged
             leptons in 139 fb −1 of √s = 13 TeV pp
             collisions with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2021},
   Number = {7},
   Year = {2021},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2021)167},
   Abstract = {A search for supersymmetry in events with four or more
             charged leptons (electrons, muons and τ-leptons) is
             presented. The analysis uses a data sample corresponding to
             139 fb−1 of proton-proton collisions delivered by the
             Large Hadron Collider at s = 13 TeV and recorded by the
             ATLAS detector. Four-lepton signal regions with up to two
             hadronically decaying τ-leptons are designed to target
             several supersymmetric models, while a general five-lepton
             signal region targets any new physics phenomena leading to a
             final state with five charged leptons. Data yields are
             consistent with Standard Model expectations and results are
             used to set upper limits on contributions from processes
             beyond the Standard Model. Exclusion limits are set at the
             95% confidence level in simplified models of general
             gauge-mediated supersymmetry, excluding higgsino masses up
             to 540 GeV. In R-parity-violating simplified models with
             decays of the lightest supersymmetric particle to charged
             leptons, lower limits of 1.6 TeV, 1.2 TeV, and 2.5 TeV are
             placed on wino, slepton and gluino masses, respectively.
             [Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP07(2021)167},
   Key = {fds366277}
}

@article{fds356670,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson,
             TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez,
             O},
   Title = {Search for supersymmetry in events with four or more leptons
             in √s =13 TeV pp collisions with ATLAS},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {3},
   Year = {2018},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.032009},
   Abstract = {Results from a search for supersymmetry in events with four
             or more charged leptons (electrons, muons and taus) are
             presented. The analysis uses a data sample corresponding to
             36.1 fb-1 of proton-proton collisions delivered by the Large
             Hadron Collider at s=13 TeV and recorded by the ATLAS
             detector. Four-lepton signal regions with up to two
             hadronically decaying taus are designed to target a range of
             supersymmetric scenarios that can be either enriched in or
             depleted of events involving the production and decay of a Z
             boson. Data yields are consistent with Standard Model
             expectations and results are used to set upper limits on the
             event yields from processes beyond the Standard Model.
             Exclusion limits are set at the 95% confidence level in
             simplified models of general gauge mediated supersymmetry,
             where Higgsino masses are excluded up to 295 GeV. In
             R-parity-violating simplified models with decays of the
             lightest supersymmetric particle to charged leptons, lower
             limits of 1.46, 1.06, and 2.25 TeV are placed on wino,
             slepton and gluino masses, respectively.},
   Doi = {10.1103/PhysRevD.98.032009},
   Key = {fds356670}
}

@article{fds310361,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for supersymmetry in events with four or more leptons
             in √s =8 TeV pp collisions with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.052001},
   Abstract = {Results from a search for supersymmetry in events with four
             or more leptons including electrons, muons and taus are
             presented. The analysis uses a data sample corresponding to
             20.3 fb-1 of proton-proton collisions delivered by the Large
             Hadron Collider at s=8 TeV and recorded by the ATLAS
             detector. Signal regions are designed to target
             supersymmetric scenarios that can be either enriched in or
             depleted of events involving the production of a Z boson. No
             significant deviations are observed in data from standard
             model predictions and results are used to set upper limits
             on the event yields from processes beyond the standard
             model. Exclusion limits at the 95% confidence level on the
             masses of relevant supersymmetric particles are obtained. In
             R-parity-violating simplified models with decays of the
             lightest supersymmetric particle to electrons and muons,
             limits of 1350 and 750 GeV are placed on gluino and chargino
             masses, respectively. In R-parity-conserving simplified
             models with heavy neutralinos decaying to a massless
             lightest supersymmetric particle, heavy neutralino masses up
             to 620 GeV are excluded. Limits are also placed on other
             supersymmetric scenarios.},
   Doi = {10.1103/PhysRevD.90.052001},
   Key = {fds310361}
}

@article{fds344667,
   Author = {The ATLAS collaboration and A and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Search for supersymmetry in events with large missing
             transverse momentum, jets, and at least one tau lepton in 20
             fb−1 of √s= 8 TeV proton-proton collision data with the
             ATLAS detector},
   Journal = {Social Psychiatry and Psychiatric Epidemiology},
   Volume = {2014},
   Number = {9},
   Publisher = {Dr. Dietrich Steinkopff Verlag GmbH and Co.
             KG},
   Year = {2014},
   url = {http://dx.doi.org/10.1007/JHEP09(2014)103},
   Abstract = {A search for supersymmetry (SUSY) in events with large
             missing transverse momentum, jets, at least one hadronically
             decaying tau lepton and zero or one additional light leptons
             (electron/muon), has been performed using 20.3fb−1of
             proton-proton collision data at √ s= 8 TeV recorded with
             the ATLAS detector at the Large Hadron Collider. No excess
             above the Standard Model background expectation is observed
             in the various signal regions and 95% confidence level upper
             limits on the visible cross section for new phenomena are
             set. The results of the analysis are interpreted in several
             SUSY scenarios, significantly extending previous limits
             obtained in the same final states. In the framework of
             minimal gauge-mediated SUSY breaking models, values of the
             SUSY breaking scale Λ below 63 TeV are excluded,
             independently of tan β. Exclusion limits are also derived
             for an mSUGRA/CMSSM model, in both the R-parity-conserving
             and R-parity-violating case. A further interpretation is
             presented in a framework of natural gauge mediation, in
             which the gluino is assumed to be the only light coloured
             sparticle and gluino masses below 1090 GeV are
             excluded.},
   Doi = {10.1007/JHEP09(2014)103},
   Key = {fds344667}
}

@article{fds307675,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Saavedra, JAA and Agustoni, M and Aharrouche,
             M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Spiers, SEA and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
             VV and Dos Santos and SPA and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik,
             E},
   Title = {Search for supersymmetry in events with large missing
             transverse momentum, jets, and at least one tau lepton in 7
             TeV proton-proton collision data with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2215-7},
   Abstract = {A search for supersymmetry (SUSY) in events with large
             missing transverse momentum, jets, and at least one
             hadronically decaying τ lepton, with zero or one additional
             light lepton (e/μ), has been performed using 4.7 fb−1of
             proton-proton collision data at √s = 7 TeV recorded with
             the ATLAS detector at the Large Hadron Collider. No excess
             above the Standard Model background expectation is observed
             and a 95 % confidence level visible cross-section upper
             limit for new phenomena is set. In the framework of
             gauge-mediated SUSY-breaking models, lower limits on the
             mass scale Λ are set at 54 TeV in the regions where the
             τ1is the next-to-lightest SUSY particle (tanβ > 20). These
             limits provide the most stringent tests to date of GMSB
             models in a large part of the parameter space
             considered.},
   Doi = {10.1140/epjc/s10052-012-2215-7},
   Key = {fds307675}
}

@article{fds307623,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
             VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, L and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos,
             S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JJB and Badescu, E and Bagnaia, P and Bahinipati,
             S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio,
             EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
             Costa, JBG and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Harpaz,
             SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni,
             A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
             M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
             R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez,
             AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi,
             G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B},
   Title = {Search for supersymmetry in events with photons, bottom
             quarks, and missing transverse momentum in proton-proton
             collisions at a centre-of-mass energy of 7 TeV with the
             ATLAS detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {719},
   Number = {4-5},
   Pages = {261-279},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.041},
   Abstract = {© 2013 CERN A search has been performed for the
             experimental signature of an isolated photon with high
             transverse momentum, at least one jet identified as
             originating from a bottom quark, and high missing transverse
             momentum. Such a final state may originate from
             supersymmetric models with gauge-mediated supersymmetry
             breaking in events in which one of a pair of higgsino-like
             neutralinos decays into a photon and a gravitino while the
             other decays into a Higgs boson and a gravitino. The search
             is performed using the full dataset of 7 TeV proton–proton
             collisions recorded with the ATLAS detector at the LHC in
             2011, corresponding to an integrated luminosity of 4.7
             fb−1. A total of 7 candidate events are observed while
             7.5±2.2 events are expected from the Standard Model
             background. The results of the search are interpreted in the
             context of general gauge mediation to exclude certain
             regions of a benchmark plane for higgsino-like neutralino
             production.},
   Doi = {10.1016/j.physletb.2013.01.041},
   Key = {fds307623}
}

@article{fds307696,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
             DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon,
             P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova,
             L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa,
             HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel,
             A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet,
             NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Booth,
             CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
             P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov,
             O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Cheplakov, A and Cherkaoui
             El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins, NJ and Collins-Tooth, C and Collot, J and Colon,
             G and Conde Muiño and P and Coniavitis, E and Conidi,
             MC},
   Title = {Search for supersymmetry in events with three leptons and
             missing transverse momentum in √[s]=7 TeV pp collisions
             with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {26},
   Pages = {261804},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.108.261804},
   Abstract = {A search for the weak production of charginos and
             neutralinos decaying to a final state with three leptons
             (electrons or muons) and missing transverse momentum is
             presented. The analysis uses 2.06 fb(-1) of √[s]=7 TeV
             proton-proton collision data delivered by the Large Hadron
             Collider and recorded with the ATLAS detector. Observations
             are consistent with standard model expectations in two
             signal regions that are either depleted or enriched in
             Z-boson decays. Upper limits at 95% confidence level are set
             in R-parity conserving phenomenological minimal
             supersymmetric and simplified models. For the simplified
             models, degenerate lightest chargino and next-to-lightest
             neutralino masses up to 300 GeV are excluded for mass
             differences from the lightest neutralino up to 300
             GeV.},
   Doi = {10.1103/physrevlett.108.261804},
   Key = {fds307696}
}

@article{fds356664,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for supersymmetry in final states with charm jets and
             missing transverse momentum in 13 TeV pp collisions with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {9},
   Year = {2018},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2018)050},
   Abstract = {A search for supersymmetric partners of top quarks decaying
             as t˜1→cχ˜10 and supersymmetric partners of charm
             quarks decaying as c˜1→cχ˜10, where χ˜10 is the
             lightest neutralino, is presented. The search uses 36.1
             fb−1pp collision data at a centre-of-mass energy of 13 TeV
             collected by the ATLAS experiment at the Large Hadron
             Collider and is performed in final states with jets
             identified as containing charm hadrons. Assuming a 100%
             branching ratio to cχ˜10, top and charm squarks with
             masses up to 850 GeV are excluded at 95% confidence level
             for a massless lightest neutralino. For mt˜1,c˜1−mχ˜10
             < 100 GeV, top and charm squark masses up to 500 GeV are
             excluded.[Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP09(2018)050},
   Key = {fds356664}
}

@article{fds307743,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for supersymmetry in final states with jets, missing
             transverse momentum and one isolated lepton in √s=7TeV pp
             collisions using 1fb -1 of ATLAS
             data},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012006},
   Abstract = {We present an update of a search for supersymmetry in final
             states containing jets, missing transverse momentum, and one
             isolated electron or muon, using 1.04fb -1 of proton-proton
             collision data at √s=7TeV recorded by the ATLAS experiment
             at the LHC in the first half of 2011. The analysis is
             carried out in four distinct signal regions with either
             three or four jets and variations on the (missing)
             transverse momentum cuts, resulting in optimized limits for
             various supersymmetry models. No excess above the standard
             model background expectation is observed. Limits are set on
             the visible cross section of new physics within the
             kinematic requirements of the search. The results are
             interpreted as limits on the parameters of the minimal
             supergravity framework, limits on cross sections of
             simplified models with specific squark and gluino decay
             modes, and limits on parameters of a model with bilinear
             R-parity violation. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.85.012006},
   Key = {fds307743}
}

@article{fds356682,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
             LJ},
   Title = {Search for supersymmetry in final states with missing
             transverse momentum and multiple b-jets in proton-proton
             collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {6},
   Year = {2018},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2018)107},
   Abstract = {A search for supersymmetry involving the pair production of
             gluinos decaying via third-generation squarks into the
             lightest neutralino (χ˜10) is reported. It uses LHC
             proton-proton collision data at a centre-of-mass energy s=13
             TeV with an integrated luminosity of 36.1 fb−1 collected
             with the ATLAS detector in 2015 and 2016. The search is
             performed in events containing large missing transverse
             momentum and several energetic jets, at least three of which
             must be identified as originating from b-quarks. To increase
             the sensitivity, the sample is divided into subsamples based
             on the presence or absence of electrons or muons. No excess
             is found above the predicted background. For χ˜10 masses
             below approximately 300 GeV, gluino masses of less than 1.97
             (1.92) TeV are excluded at 95% confidence level in
             simplified models involving the pair production of gluinos
             that decay via top (bottom) squarks. An interpretation of
             the limits in terms of the branching ratios of the gluinos
             into third-generation squarks is also provided. These
             results improve upon the exclusion limits obtained with the
             3.2 fb−1 of data collected in 2015.[Figure not available:
             see fulltext.].},
   Doi = {10.1007/JHEP06(2018)107},
   Key = {fds356682}
}

@article{fds374215,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
             A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
             W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
             PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
             Ferraz, V and Arcangeletti, C and Arce, ATH and Arena,
             E},
   Title = {Search for supersymmetry in final states with missing
             transverse momentum and three or more b-jets in 139
             fb-1 of proton–proton collisions at √s=13 TeV
             with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {7},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2023},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11543-6},
   Abstract = {A search for supersymmetry involving the pair production of
             gluinos decaying via off-shell third-generation squarks into
             the lightest neutralino (χ~10) is reported. It exploits LHC
             proton–proton collision data at a centre-of-mass energy
             s=13 TeV with an integrated luminosity of 139 fb - 1
             collected with the ATLAS detector from 2015 to 2018. The
             search uses events containing large missing transverse
             momentum, up to one electron or muon, and several energetic
             jets, at least three of which must be identified as
             containing b-hadrons. Both a simple kinematic event
             selection and an event selection based upon a deep
             neural-network are used. No significant excess above the
             predicted background is found. In simplified models
             involving the pair production of gluinos that decay via
             off-shell top (bottom) squarks, gluino masses less than
             2.44 TeV (2.35 TeV) are excluded at 95% CL for a massless
             χ~10. Limits are also set on the gluino mass in models with
             variable branching ratios for gluino decays to
             bb¯χ~10,tt¯χ~10 and tb¯χ~1-/t¯bχ~1+.},
   Doi = {10.1140/epjc/s10052-023-11543-6},
   Key = {fds374215}
}

@article{fds356738,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham,
             NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
             P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Search for supersymmetry in final states with two same-sign
             or three leptons and jets using 36 fb−1 of
             √s=13 TeV pp collision data with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {9},
   Year = {2017},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2017)084},
   Abstract = {A search for strongly produced supersymmetric particles
             using signatures involving multiple energetic jets and
             either two isolated same-sign leptons (e or μ), or at least
             three isolated leptons, is presented. The analysis relies on
             the identification of b-jets and high missing transverse
             momentum to achieve good sensitivity. A data sample of
             proton-proton collisions at s=13 TeV recorded with the ATLAS
             detector at the Large Hadron Collider in 2015 and 2016,
             corresponding to a total integrated luminosity of 36.1
             fb−1, is used for the search. No significant excess over
             the Standard Model prediction is observed. The results are
             interpreted in several simplified supersymmetric models
             featuring R-parity conservation or R-parity violation,
             extending the exclusion limits from previous searches. In
             models considering gluino pair production, gluino masses are
             excluded up to 1.87 TeV at 95% confidence level. When bottom
             squarks are pair-produced and decay to a chargino and a top
             quark, models with bottom squark masses below 700 GeV and
             light neutralinos are excluded at 95% confidence level. In
             addition, model-independent limits are set on a possible
             contribution of new phenomena to the signal region
             yields.[Figure not available: see fulltext.].},
   Doi = {10.1007/JHEP09(2017)084},
   Key = {fds356738}
}

@article{fds307782,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Search for supersymmetry in pp collisions at √s=7TeV in
             final states with missing transverse momentum and b-jets
             with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.112006},
   Abstract = {The results of a search for supersymmetry in events with
             large missing transverse momentum and heavy-flavor jets
             using an integrated luminosity corresponding to 2.05fb-1 of
             pp collisions at √s=7TeV recorded with the ATLAS detector
             at the Large Hadron Collider are reported. No significant
             excess is observed with respect to the prediction for
             standard model processes. Results are interpreted in a
             variety of R-parity conserving models in which scalar
             bottoms and tops are the only scalar quarks to appear in the
             gluino decay cascade, and in an SO(10) model framework.
             Gluino masses up to 600-900GeV are excluded, depending on
             the model considered. © 2012 CERN. Published by the
             American Physical Society.},
   Doi = {10.1103/PhysRevD.85.112006},
   Key = {fds307782}
}

@article{fds308002,
   Author = {Aaltonen, T and others},
   Title = {Search for Supersymmetry in pp̅ Collisions at √ s
             =1.96 TeV Using the Trilepton Signature for
             Chargino-Neutralino Production},
   Journal = {Physical Review Letters},
   Volume = {101},
   Number = {25},
   Pages = {251801},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.251801},
   Abstract = {We use the three lepton and missing energy trilepton
             signature to search for chargino-neutralino production with
             2.0  fb-1 of integrated luminosity collected by the CDF
             II experiment at the Tevatron pp̅ collider. We expect an
             excess of approximately 11 supersymmetric events for a
             choice of parameters of the mSUGRA model, but our
             observation of 7 events is consistent with the standard
             model expectation of 6.4 events. We constrain the mSUGRA
             model of supersymmetry and rule out chargino masses up to
             145  GeV/c2 for a specific choice of
             parameters.},
   Doi = {10.1103/physrevlett.101.251801},
   Key = {fds308002}
}

@article{fds308137,
   Author = {Abazov, VM and Abbott, B and Abolins, M and Acharya, BS and Adams, DL and Adams, M and Adams, T and Agelou, M and Agram, J-L and Ahmed, SN and Ahn,
             SH and Alexeev, GD and Alkhazov, G and Alton, A and Alverson, G and Alves,
             GA and Anderson, S and Andrieu, B and Arnoud, Y and Askew, A and Asman, B and Atramentov, O and Autermann, C and Avila, C and Babukhadia, L and Bacon,
             TC and Baden, A and Baffioni, S and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Bargassa, P and Baringer, P and Barnes, C and Barreto,
             J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beauceron,
             S and Beaudette, F and Begel, M and Bellavance, A and Beri, SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Besson,
             A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Binder, M and Bischoff, A and Black, KM and Blackler, I and Blazey, G and Blekman, F and Bloch, D and Blumenschein,
             U and Boehnlein, A and Boeriu, O and Bolton, TA and Bonamy, P and Borcherding, F and Borissov, G and Bos, K and Bose, T and Boswell, C and Brandt, A and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchanan, NJ and Buchholz, D and Buehler, M and Buescher, V and Burdin,
             S and Burnett, TH and Busato, E and Butler, JM and Bystricky, J and Canelli, F and Carvalho, W and Casey, BCK and Casey, D and Cason, NM and Castilla-Valdez, H and Chakrabarti, S and Chakraborty, D and Chan,
             KM and Chandra, A and Chapin, D and Charles, F and Cheu, E and Chevalier,
             L and Cho, DK and Choi, S and Chopra, S and Christiansen, T and Christofek,
             L and Claes, D and Clark, AR and Clément, B and Clément, C and Coadou, Y and Colling, DJ and Coney, L and Connolly, B and Cooke, M and Cooper, WE and Coppage, D and Corcoran, M and Coss, J and Cothenet, A and Cousinou,
             M-C and Crépé-Renaudin, S and Cristetiu, M and Cummings, MAC and Cutts, D and da Motta, H and Davies, B and Davies, G and Davis, GA and De,
             K and de Jong, P and de Jong, SJ and De La Cruz-Burelo and E and De
             Oliveira Martins and C and Dean, S and Del Signore and K and Déliot, F and Delsart, PA and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doidge, M and Dong, H and Doulas, S and Duflot, L and Dugad, SR and Duperrin, A and Dyer,
             J and Dyshkant, A and Eads, M and Edmunds, D and Edwards, T and Ellison, J and Elmsheuser, J and Eltzroth, JT and Elvira, VD and Eno, S and Ermolov, P and Eroshin, OV and Estrada, J and Evans, D and Evans, H and Evdokimov, A and Evdokimov, VN and Fast, J and Fatakia, SN and Fein, D and Feligioni, L and Ferbel, T and Fiedler, F and Filthaut, F and Fisher, W and Fisk, HE and Fleuret, F and Fortner, M and Fox, H and Freeman, W and Fu, S and Fuess, S and Galea, CF and Gallas, E and Galyaev, E and Gao, M and Garcia, C and Garcia-Bellido, A and Gardner, J and Gavrilov, V and Gelé, D and Gelhaus, R and Genser, K and Gerber, CE and Gershtein, Y and Geurkov, G and Ginther, G and Goldmann, K and Golling, T and Gómez, B and Gounder, K and Goussiou, A and Graham, G and Grannis, PD and Greder, S and Green, JA and Greenlee, H and Greenwood, ZD and Gregores, EM and Grinstein, S and Grivaz, J-F and Groer, L and Grünendahl, S and Grünewald, MW and Gu,
             W and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Haas, A and Hadley, NJ and Haggerty, H and Hagopian, S and Hall, I and Hall, RE and Han, C and Han, L and Hanagaki, K and Hanlet, P and Harder, K and Harrington, R and Hauptman, JM and Hauser, R and Hays, C and Hays, J and Hebbeker, T and Hebert, C and Hedin, D and Heinmiller, JM and Heinson,
             AP and Heintz, U and Hensel, C and Hesketh, G and Hildreth, MD and Hirosky,
             R and Hobbs, JD and Hoeneisen, B and Hohlfeld, M and Hong, SJ and Hooper,
             R and Hou, S and Hu, Y and Huang, J and Huang, Y and Iashvili, I and Illingworth, R and Ito, AS and Jabeen, S and Jaffré, M and Jain, S and Jain, V and Jakobs, K and Jenkins, A and Jesik, R and Jiang, Y and Johns,
             K and Johnson, M and Johnson, P and Jonckheere, A and Jonsson, P and Jöstlein, H and Juste, A and Kado, MM and Käfer, D and Kahl, W and Kahn,
             S and Kajfasz, E and Kalinin, AM and Kalk, J and Karmanov, D and Kasper, J and Kau, D and Ke, Z and Kehoe, R and Kermiche, S and Kesisoglou, S and Khanov,
             A and Kharchilava, A and Kharzheev, YM and Kim, KH and Klima, B and Klute,
             M and Kohli, JM and Kopal, M and Korablev, VM and Kotcher, J and Kothari,
             B and Kotwal, AV and Koubarovsky, A and Kouchner, A and Kouznetsov, O and Kozelov, AV and Kozminski, J and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kurca, T and Kuznetsov, VE and Lager, S and Lahrichi, N and Landsberg, G and Lazoflores, J and Le Bihan and A-C and Lebrun, P and Lee, SW and Lee, WM and Leflat, A and Leggett, C and Lehner,
             F and Leonidopoulos, C and Lewis, P and Li, J and Li, QZ and Li, X and Lima,
             JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipaev, VV and Lipton,
             R and Lobo, L and Lobodenko, A and Lokajicek, M and Lounis, A and Lu, J and Lubatti, HJ and Lucotte, A and Lueking, L and Luo, C and Lynker, M and Lyon, AL and Maciel, AKA and Madaras, RJ and Mättig, P and Magerkurth,
             A and Magnan, A-M and Maity, M and Mal, PK and Malik, S and Malyshev, VL and Manankov, V and Mao, HS and Maravin, Y and Marshall, T and Martens, M and Martin, MI and Mattingly, SEK and Mayorov, AA and McCarthy, R and McCroskey, R and McMahon, T and Meder, D and Melanson, HL and Melnitchouk, A and Meng, X and Merkin, M and Merritt, KW and Meyer, A and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mitrevski,
             J and Mokhov, N and Molina, J and Mondal, NK and Montgomery, HE and Moore,
             RW and Mostafa, M and Muanza, GS and Mulders, M and Mutaf, YD and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Naumann, NA and Neal, HA and Negret, JP and Nelson, S and Neustroev, P and Noeding, C and Nomerotski,
             A and Novaes, SF and Nunnemann, T and Nurse, E and O'Dell, V and O'Neil,
             DC and Oguri, V and Oliveira, N and Olivier, B and Oshima, N and Otero y
             Garzón, GJ and Padley, P and Papageorgiou, K and Parashar, N and Park,
             J and Park, SK and Parsons, J and Partridge, R and Parua, N and Patwa, A and Perea, PM and Perez, E and Peters, O and Pétroff, P and Petteni, M and Phaf, L and Piegaia, R and Podesta-Lerma, PLM and Podstavkov, VM and Pope, BG and Popkov, E and Prado da Silva and WL and Prosper, HB and Protopopescu, S and Przybycien, MB and Qian, J and Quadt, A and Quinn,
             B and Rani, KJ and Rapidis, PA and Ratoff, PN and Reay, NW and Renardy,
             J-F and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Ripp-Baudot, I and Rizatdinova, F and Royon, C and Rubinov, P and Ruchti, R and Sabirov, BM and Sajot, G and Sánchez-Hernández, A and Sanders, MP and Santoro, A and Savage, G and Sawyer, L and Scanlon, T and Schamberger, RD and Schellman, H and Schieferdecker, P and Schmitt,
             C and Schukin, AA and Schwartzman, A and Schwienhorst, R and Sengupta,
             S and Severini, H and Shabalina, E and Shary, V and Shephard, WD and Shpakov, D and Sidwell, RA and Simak, V and Sirotenko, V and Skow, D and Skubic, P and Slattery, P and Smith, RP and Smolek, K and Snow, GR and Snow, J and Snyder, S and Söldner-Rembold, S and Song, X and Song, Y and Sonnenschein, L and Sopczak, A and Sorín, V and Sosebee, M and Soustruznik, K and Souza, M and Spurlock, B and Stanton, NR and Stark,
             J and Steele, J and Steinbrück, G and Stevenson, K and Stolin, V and Stone, A and Stoyanova, DA and Strandberg, J},
   Title = {Search for supersymmetry with gauge-mediated breaking in
             diphoton events at D0.},
   Journal = {Physical review letters},
   Volume = {94},
   Number = {4},
   Pages = {041801},
   Year = {2005},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.94.041801},
   Abstract = {We report the results of a search for supersymmetry (SUSY)
             with gauge-mediated breaking in the missing transverse
             energy distribution of inclusive diphoton events using 263
             pb(-1) of data collected by the D0 experiment at the
             Fermilab Tevatron Collider in 2002-2004. No excess is
             observed above the background expected from standard model
             processes, and lower limits on the masses of the lightest
             neutralino and chargino of about 108 and 195 GeV,
             respectively, are set at the 95% confidence level. These are
             the most stringent limits to date for models with
             gauge-mediated SUSY breaking with a short-lived neutralino
             as the next-to-lightest SUSY particle.},
   Doi = {10.1103/physrevlett.94.041801},
   Key = {fds308137}
}

@article{fds307913,
   Author = {Aaltonen, and T, and others},
   Title = {Search for Supersymmetry with Gauge-Mediated Breaking in
             Diphoton Events with Missing Transverse Energy at CDF
             II},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {1},
   Pages = {011801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.011801},
   Abstract = {http://arxiv.org/abs/0910.3606},
   Doi = {10.1103/PhysRevLett.104.011801},
   Key = {fds307913}
}

@article{fds307779,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Search for supersymmetry with jets, missing transverse
             momentum and at least one hadronically decaying τ lepton in
             proton-proton collisions at s=7TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {714},
   Number = {2-5},
   Pages = {197-214},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {August},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.06.061},
   Abstract = {A search for production of supersymmetric particles in final
             states containing jets, missing transverse momentum, and at
             least one hadronically decaying τ lepton is presented. The
             data were recorded by the ATLAS experiment in s=7TeV
             proton-proton collisions at the Large Hadron Collider. No
             excess above the Standard Model background expectation was
             observed in 2.05fb-1 of data. The results are interpreted in
             the context of gauge mediated supersymmetry breaking models
             with Mmess=250TeV, N5=3, μ>0, and Cgrav=1. The production
             of supersymmetric particles is excluded at 95% C.L. up to a
             supersymmetry breaking scale Λ=30TeV, independent of tanβ,
             and up to Λ=43TeV for large tanβ. © 2012.},
   Doi = {10.1016/j.physletb.2012.06.061},
   Key = {fds307779}
}

@article{fds307653,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and d'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucà, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
             N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Search for supersymmetry with like-sign lepton-tau events at
             CDF.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {20},
   Pages = {201802},
   Year = {2013},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.110.201802},
   Abstract = {We present a search for chargino-neutralino associated
             production using like electric charge dilepton events
             collected by the CDF II detector at the Fermilab Tevatron in
             proton-antiproton collisions at sqrt[s] = 1.96 TeV. One
             lepton is identified as the hadronic decay of a tau lepton,
             while the other is an electron or muon. In data
             corresponding to 6.0 fb(-1) of integrated luminosity, we
             obtain good agreement with standard model predictions and
             set limits on the chargino-neutralino production cross
             section for simplified gravity- and gauge-mediated models.
             As an example, assuming that the chargino and neutralino
             decays to taus dominate, in the simplified gauge-mediated
             model we exclude cross sections greater than 300 fb at 95%
             credibility level for chargino and neutralino masses of 225
             GeV/c(2). This analysis is the first to extend the LHC
             searches for electroweak supersymmetric production of
             gauginos to high tanβ and slepton next-to-lightest
             supersymmetric particle scenarios.},
   Doi = {10.1103/physrevlett.110.201802},
   Key = {fds307653}
}

@article{fds307689,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
             PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas,
             CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
             X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC},
   Title = {Search for tb resonances in proton-proton collisions at
             √s=7 TeV with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {8},
   Pages = {081801},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.109.081801},
   Abstract = {This Letter presents a search for tb resonances in 1.04
             fb(-1) of LHC proton-proton collision data collected by the
             ATLAS detector at a center-of-mass energy of 7 TeV. Events
             with a lepton, missing transverse momentum, and two jets are
             selected and the invariant mass of the corresponding final
             state is reconstructed. The search exploits the shape of the
             tb invariant mass distribution compared to the expected
             standard model backgrounds. The model of a right-handed
             W(R)' with standard model-like couplings is chosen as the
             benchmark model for this search. No statistically
             significant excess of events is observed in the data, and
             upper limits on the cross section times the branching ratio
             of W(R)' resonances at 95% C.L. lie in the range of 6.1-1.0
             pb for W(R)' masses ranging from 0.5 to 2.0 TeV. These
             limits are translated into a lower bound on the allowed
             right-handed W(R)' mass, giving m(W(R)'))>1.13 TeV at 95%
             C.L.},
   Doi = {10.1103/physrevlett.109.081801},
   Key = {fds307689}
}

@article{fds307907,
   Author = {Aaltonen, and T, and others},
   Title = {Search for Technicolor Particles Produced in Association
             with a $W$ Boson at CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {11},
   Pages = {111802},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.111802},
   Abstract = {http://arxiv.org/abs/0912.2059},
   Doi = {10.1103/PhysRevLett.104.111802},
   Key = {fds307907}
}

@article{fds307724,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli,
             EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
             N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
             R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana,
             S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
             J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani,
             G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Search for TeV-scale gravity signatures in final states with
             leptons and jets with the ATLAS detector at √ s=7
             TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {716},
   Number = {1},
   Pages = {122-141},
   Publisher = {Elsevier BV},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.08.009},
   Abstract = {The production of events with multiple high transverse
             momentum particles including charged leptons and jets is
             measured, using 1.04 fb-1 of proton-proton collision data
             recorded by the ATLAS detector during the first half of 2011
             at √s=7 TeV. No excess beyond Standard Model expectations
             is observed, and upper limits on the fiducial cross sections
             for non-Standard Model production of these final states are
             set. Using models for string ball and black hole production
             and decay, exclusion contours are determined as a function
             of mass threshold and the fundamental gravity scale. © 2012
             CERN.},
   Doi = {10.1016/j.physletb.2012.08.009},
   Key = {fds307724}
}

@article{fds321087,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Search for TeV-scale gravity signatures in high-mass final
             states with leptons and jets with the ATLAS detector at
             √s=13 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {760},
   Pages = {520-537},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.07.030},
   Abstract = {A search for physics beyond the Standard Model, in final
             states with at least one high transverse momentum charged
             lepton (electron or muon) and two additional high transverse
             momentum leptons or jets, is performed using 3.2 fb−1 of
             proton–proton collision data recorded by the ATLAS
             detector at the Large Hadron Collider in 2015 at s=13 TeV.
             The upper end of the distribution of the scalar sum of the
             transverse momenta of leptons and jets is sensitive to the
             production of high-mass objects. No excess of events beyond
             Standard Model predictions is observed. Exclusion limits are
             set for models of microscopic black holes with two to six
             extra dimensions.},
   Doi = {10.1016/j.physletb.2016.07.030},
   Key = {fds321087}
}

@article{fds313599,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for the associated production of the Higgs boson with
             a top quark pair in multilepton final states with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {749},
   Pages = {519-541},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {October},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.07.079},
   Abstract = {A search for the associated production of the Higgs boson
             with a top quark pair is performed in multilepton final
             states using 20.3 fb−1 of proton–proton collision data
             recorded by the ATLAS experiment at s=8 TeV at the Large
             Hadron Collider. Five final states, targeting the decays
             H→WW⁎, ττ, and ZZ⁎, are examined for the presence of
             the Standard Model (SM) Higgs boson: two same-charge light
             leptons (e or μ) without a hadronically decaying τ lepton;
             three light leptons; two same-charge light leptons with a
             hadronically decaying τ lepton; four light leptons; and one
             light lepton and two hadronically decaying τ leptons. No
             significant excess of events is observed above the
             background expectation. The best fit for the tt¯H
             production cross section, assuming a Higgs boson mass of 125
             GeV, is 2.1−1.2+1.4 times the SM expectation, and the
             observed (expected) upper limit at the 95% confidence level
             is 4.7 (2.4) times the SM rate. The p-value for
             compatibility with the background-only hypothesis is 1.8σ;
             the expectation in the presence of a Standard Model signal
             is 0.9σ.},
   Doi = {10.1016/j.physletb.2015.07.079},
   Key = {fds313599}
}

@article{fds307936,
   Author = {Aaltonen, T and others},
   Title = {Search for the Associated Production of the Standard-Model
             Higgs Boson in the All-Hadronic Channel},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {22},
   Pages = {221801},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.221801},
   Abstract = {We report on a search for the standard-model Higgs boson in
             pp̅ collisions at sqrt[s]=1.96  TeV using an integrated
             luminosity of 2.0  fb-1. We look for production of the
             Higgs boson decaying to a pair of bottom quarks in
             association with a vector boson V (W or Z) decaying to
             quarks, resulting in a four-jet final state. Two of the jets
             are required to have secondary vertices consistent with
             B-hadron decays. We set the first 95% confidence level upper
             limit on the VH production cross section with V(→qq̅
             /qq′)H(→bb̅ ) decay for Higgs boson masses of
             100--150  GeV/c2 using data from run II at the Fermilab
             Tevatron. For mH=120  GeV/c2, we exclude cross sections
             larger than 38 times the standard-model prediction.},
   Doi = {10.1103/physrevlett.103.221801},
   Key = {fds307936}
}

@article{fds310325,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Search for the b¯b decay of the Standard Model Higgs boson
             in associated (W/Z)H production with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2015)069},
   Abstract = {Abstract: A search for the (Formula presented.) decay of the
             Standard Model Higgs boson is performed with the ATLAS
             experiment using the full dataset recorded at the LHC in Run
             1. The integrated luminosities used are 4.7 and 20.3 fb−1
             from pp collisions at (Formula presented.) and 8 TeV,
             respectively. The processes considered are associated (W/Z)H
             production, where W → eν/μν, Z → ee/μμ and Z →
             νν. The observed (expected) deviation from the
             background-only hypothesis corresponds to a significance of
             1.4 (2.6) standard deviations and the ratio of the measured
             signal yield to the Standard Model expectation is found to
             be μ = 0.52 ± 0.32 (stat.) ± 0.24 (syst.) for a Higgs
             boson mass of 125.36 GeV. The analysis procedure is
             validated by a measurement of the yield of (W/Z)Z production
             with (Formula presented.) in the same final states as for
             the Higgs boson search, from which the ratio of the observed
             signal yield to the Standard Model expectation is found to
             be 0.74 ± 0.09 (stat.) ± 0.14 (syst.).[Figure not
             available: see fulltext.].},
   Doi = {10.1007/JHEP01(2015)069},
   Key = {fds310325}
}

@article{fds373911,
   Author = {Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Sharma, AS and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Belfkir, M and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Franco, L and Goy, C and Guillemin,
             T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Lafaye, R and Levêque, J and Lorenzo Martinez and N and Portales, L and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Wingerter-Seez, I and Abulaiti, Y and Bhopatkar, VS and Chekanov, S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe,
             J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Zhang, J and Berlendis, S and Cheu, E and Delitzsch, CM and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas,
             JCJ and De, K and Eifert, T and Farbin, A and Hadavand, HK and Little, JD and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Gazis, EN and Gkountoumis, P and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Perini, L and Tzanis, P and Zacharis, G and Andeen, T and Burton, CD and Choi, K and Nikiforou, N and Onyisi, PUE and Panchal, DK and Roy, A and Unal, M and Webb, AF and Beddall, AJ and Celebi, E},
   Title = {Search for the charged-lepton-flavor-violating decay Z →
             eμ in pp collisions at √s = 13 TeV ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {108},
   Number = {3},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.108.032015},
   Abstract = {A search for the charged-lepton-flavor-violating process
             Formula Presented is presented, using Formula Presented of
             Formula Presented Formula Presented collision data collected
             by the ATLAS experiment at the LHC. An excess in the Formula
             Presented invariant mass spectrum near the Formula Presented
             boson mass would be a striking signature of new physics. No
             excess is observed, and an upper limit Formula Presented is
             placed on the branching fraction at 95% confidence level,
             which is the most stringent limit to date.},
   Doi = {10.1103/PhysRevD.108.032015},
   Key = {fds373911}
}

@booklet{Abbott98i,
   Author = {B. Abbott and M. Abolins and B. S. Acharya and I. Adam and D. L. Adams and M. Adams and S. Ahn and H. Aihara and G. A.
             Alves and N. Amos and E. W. Anderson and R. Astur and M. M.
             Baarmand and A. Baden and V. Balamurali and J. Balderston and B. Baldin and},
   Title = {Search for the decay b -$>$ X-s mu(+)mu(-)},
   Journal = {Physics Letters B},
   Volume = {423},
   Number = {3-4},
   Pages = {419 -- 426},
   Year = {1998},
   Month = {March},
   Key = {Abbott98i}
}

@article{fds313624,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau,
             M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio,
             EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
             JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
             S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans,
             G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins, NJ and Collins-Tooth, C and Collot,
             J and Colon, G and Muiño, PC and Coniavitis, E and Conidi, MC and Consonni, SM and Consorti, V},
   Title = {Search for the decay Bs0→μ+μ-
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {713},
   Number = {4-5},
   Pages = {387-407},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.06.013},
   Abstract = {A blind analysis searching for the decay Bs0→μ+μ- has
             been performed using proton-proton collisions at a
             centre-of-mass energy of 7 TeV recorded with the ATLAS
             detector at the LHC. With an integrated luminosity of 2.4
             fb-1 no excess of events over the background expectation is
             found and an upper limit is set on the branching fraction
             BR(Bs0→μ+μ-)&lt;2.2(1.9)×10-8 at 95% (90%) confidence
             level. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.06.013},
   Key = {fds313624}
}

@article{fds376246,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
             SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
             CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
   Title = {Search for the decay of the Higgs boson to a Z boson and a
             light pseudoscalar particle decaying to two
             photons},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {850},
   Year = {2024},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2024.138536},
   Abstract = {A search for the decay of the Higgs boson to a Z boson and a
             light, pseudoscalar particle, a, decaying respectively to
             two leptons and to two photons is reported. The search uses
             the full LHC Run 2 proton–proton collision data at s=13
             TeV, corresponding to 139 fb−1 collected by the ATLAS
             detector. This is one of the first searches for this
             specific decay mode of the Higgs boson, and it probes
             unexplored parameter space in models with axion-like
             particles (ALPs) and extended scalar sectors. The mass of
             the a particle is assumed to be in the range 0.1–33 GeV.
             The data are analysed in two categories: a merged category
             where the photons from the a decay are reconstructed in the
             ATLAS calorimeter as a single cluster, and a resolved
             category in which two separate photons are detected. The
             main background processes are from Standard Model Z boson
             production in association with photons or jets. The data are
             in agreement with the background predictions, and upper
             limits on the branching ratio of the Higgs boson decay to Za
             times the branching ratio a→γγ are derived at the 95%
             confidence level and they range from 0.08% to 2% depending
             on the mass of the a particle. The results are also
             interpreted in the context of ALP models.},
   Doi = {10.1016/j.physletb.2024.138536},
   Key = {fds376246}
}

@article{fds347461,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
             M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
             J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez,
             O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines,
             JT and Bajic, M and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnea,
             R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary,
             O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
             NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini,
             C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black,
             JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boerner,
             D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona,
             M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau,
             JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow,
             TM and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
             D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
             Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară,
             IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Clark,
             A and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M},
   Title = {Search for the Decay of the Higgs Boson to Charm Quarks with
             the ATLAS Experiment.},
   Journal = {Physical review letters},
   Volume = {120},
   Number = {21},
   Pages = {211802},
   Year = {2018},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.120.211802},
   Abstract = {A direct search for the standard model Higgs boson decaying
             to a pair of charm quarks is presented. Associated
             production of the Higgs and Z bosons, in the decay mode
             ZH→ℓ^{+}ℓ^{-}cc[over ¯] is studied. A data set with
             an integrated luminosity of 36.1  fb^{-1} of pp
             collisions at sqrt[s]=13TeV recorded by the ATLAS experiment
             at the LHC is used. The H→cc[over ¯] signature is
             identified using charm-tagging algorithms. The observed
             (expected) upper limit on σ(pp→ZH)×B(H→cc[over ¯]) is
             2.7 (3.9_{-1.1}^{+2.1}) pb at the 95% confidence level for
             a Higgs boson mass of 125 GeV, while the standard model
             value is 26 fb.},
   Doi = {10.1103/physrevlett.120.211802},
   Key = {fds347461}
}

@article{fds307952,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
             S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni,
             GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest,
             R and Frank, MJ and Franklin, M and Freeman, JC and Furic, I and Gallinaro,
             M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
             M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber,
             C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
             RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll,
             J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Griso, SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Rutherford, B and Saarikko, H and Safonov, A and Sakumoto,
             WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla,
             A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D},
   Title = {Search for the decays B_{(s)};{0} --> e;{+} micro;{-} and
             B_{(s)};{0} --> e;{+} e;{-} in CDF run II.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {20},
   Pages = {201801},
   Year = {2009},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.102.201801},
   Abstract = {We report results from a search for the lepton flavor
             violating decays B_{s};{0} --> e;{+} micro;{-} and B;{0} -->
             e;{+} micro;{-}, and the flavor-changing neutral-current
             decays B_{s};{0} --> e;{+} e;{-} and B;{0} --> e;{+} e;{-}.
             The analysis uses data corresponding to 2 fb;{-1} of
             integrated luminosity of pp[over ] collisions at sqrt[s] =
             1.96 TeV collected with the upgraded Collider Detector (CDF
             II) at the Fermilab Tevatron. The observed number of B0 and
             B_{s};{0} candidates is consistent with background
             expectations. The resulting Bayesian upper limits on the
             branching ratios at 90% credibility level are B(B_{s};{0}
             --> e;{+} micro;{-}) < 2.0 x 10;{-7}, B(B;{0} --> e;{+}
             micro;{-}) < 6.4 x 10;{-8}, B(B_{s};{0} --> e;{+} e;{-}) <
             2.8 x 10;{-7}, and B(B;{0} --> e;{+} e;{-}) < 8.3 x 10;{-8}.
             From the limits on B(B_{(s)};{0} --> e;{+} micro;{-}), the
             following lower bounds on the Pati-Salam leptoquark masses
             are also derived: M_{LQ}(B_{s};{0} --> e;{+} micro;{-}) >
             47.8 TeV/c;{2}, and M_{LQ}(B;{0} --> e;{+} micro;{-}) > 59.3
             TeV / c;{2}, at 90% credibility level.},
   Doi = {10.1103/physrevlett.102.201801},
   Key = {fds307952}
}

@article{fds347488,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines,
             JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann,
             TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
             NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
             TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
             A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ},
   Title = {Search for the Dimuon Decay of the Higgs Boson in pp
             Collisions at sqrt[s]=13  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {119},
   Number = {5},
   Pages = {051802},
   Year = {2017},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.119.051802},
   Abstract = {A search for the dimuon decay of the Higgs boson was
             performed using data corresponding to an integrated
             luminosity of 36.1  fb^{-1} collected with the ATLAS
             detector in pp collisions at sqrt[s]=13  TeV at the
             Large Hadron Collider. No significant excess is observed
             above the expected background. The observed (expected) upper
             limit on the cross section times branching ratio is 3.0
             (3.1) times the Standard Model prediction at the
             95% confidence level for a Higgs boson mass of 125 GeV.
             When combined with the pp collision data at
             sqrt[s]=7  TeV and sqrt[s]=8  TeV, the observed
             (expected) upper limit is 2.8 (2.9) times the Standard Model
             prediction.},
   Doi = {10.1103/physrevlett.119.051802},
   Key = {fds347488}
}

@article{fds347468,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
             NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
             de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
             YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
             YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou,
             Y},
   Title = {Search for the direct production of charginos and
             neutralinos in final states with tau leptons in s = 13 TeV
             pp collisions with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {78},
   Number = {2},
   Pages = {154},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-018-5583-9},
   Abstract = {A search for the direct production of charginos and
             neutralinos in final states with at least two hadronically
             decaying tau leptons is presented. The analysis uses a
             dataset of <i>pp</i> collisions corresponding to an
             integrated luminosity of 36.1 fb - 1 , recorded with the
             ATLAS detector at the Large Hadron Collider at a
             centre-of-mass energy of 13 TeV. No significant deviation
             from the expected Standard Model background is observed.
             Limits are derived in scenarios of pair production and of
             and production in simplified models where the neutralinos
             and charginos decay solely via intermediate left-handed
             staus and tau sneutrinos, and the mass of the τ ~ L state
             is set to be halfway between the masses of the and the .
             Chargino masses up to 630 GeV are excluded at 95% confidence
             level in the scenario of direct production of for a massless
             . Common and masses up to 760 GeV are excluded in the case
             of production of and assuming a massless . Exclusion limits
             for additional benchmark scenarios with large and small
             mass-splitting between the and the are also studied by
             varying the τ ~ L mass between the masses of the and the
             .},
   Doi = {10.1140/epjc/s10052-018-5583-9},
   Key = {fds347468}
}

@article{fds313590,
   Author = {The, ATLASC and Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J},
   Title = {Search for the direct production of charginos, neutralinos
             and staus in final states with at least two hadronically
             decaying taus and missing transverse momentum in pp
             collisions at √ $$ \sqrt{s}=8 $$ TeV with the ATLAS
             detector},
   Journal = {Critical Ultrasound Journal},
   Volume = {2014},
   Number = {10},
   Year = {2014},
   Month = {January},
   ISSN = {1126-6708},
   url = {http://dx.doi.org/10.1007/JHEP10(2014)096},
   Abstract = {© 2014, The Author(s).Abstract: Results of a search for the
             electroweak associated production of charginos and
             next-to-lightest neutralinos, pairs of charginos or pairs of
             tau sleptons are presented. These processes are
             characterised by final states with at least two hadronically
             decaying tau leptons, missing transverse momentum and low
             jet activity. The analysis is based on an integrated
             luminosity of 20.3 fb−1 of proton-proton collisions at
             (Formula presented) recorded with the ATLAS experiment at
             the Large Hadron Collider. No significant excess is observed
             with respect to the predictions from Standard Model
             processes. Limits are set at 95% confidence level on the
             masses of the lighter chargino and next-to-lightest
             neutralino for various hypotheses for the lightest
             neutralino mass in simplified models. In the scenario of
             direct production of chargino pairs, with each chargino
             decaying into the lightest neutralino via an intermediate
             tau slepton, chargino masses up to 345 GeV are excluded for
             a massless lightest neutralino. For associated production of
             mass-degenerate charginos and next-to-lightest neutralinos,
             both decaying into the lightest neutralino via an
             intermediate tau slepton, masses up to 410 GeV are excluded
             for a massless lightest neutralino.[Figure not available:
             see fulltext.]},
   Doi = {10.1007/JHEP10(2014)096},
   Key = {fds313590}
}

@article{fds356778,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for the electroweak production of supersymmetric
             particles in √s = 8 TeV pp collisions with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {5},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.052002},
   Abstract = {The ATLAS experiment has performed extensive searches for
             the electroweak production of charginos, neutralinos, and
             staus. This article summarizes and extends the search for
             electroweak supersymmetry with new analyses targeting
             scenarios not covered by previously published searches. New
             searches use vector-boson fusion production, initial-state
             radiation jets, and low-momentum lepton final states, as
             well as multivariate analysis techniques to improve the
             sensitivity to scenarios with small mass splittings and
             low-production cross sections. Results are based on 20 fb-1
             of proton-proton collision data at √s = 8 TeV recorded
             with the ATLAS experiment at the Large Hadron Collider. No
             significant excess beyond Standard Model expectations is
             observed. The new and existing searches are combined and
             interpreted in terms of 95% confidence-level exclusion
             limits in simplified models, where a single production
             process and decay mode is assumed, as well as within
             phenomenological supersymmetric models.},
   Doi = {10.1103/PhysRevD.93.052002},
   Key = {fds356778}
}

@article{fds356687,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo,
             N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Galloni, C and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo,
             S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà,
             A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak,
             R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino,
             P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon,
             CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat,
             P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano,
             I and Napier, A and Nett, J and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Okusawa, T and Orava,
             R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
             C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
             K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfmeister, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu,
             GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Search for the Exotic Meson X(5568) with the Collider
             Detector at Fermilab.},
   Journal = {Physical review letters},
   Volume = {120},
   Number = {20},
   Pages = {202006},
   Year = {2018},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.120.202006},
   Abstract = {A search for the exotic meson X(5568) decaying into the
             B_{s}^{0}π^{±} final state is performed using data
             corresponding to 9.6  fb^{-1} from pp[over ¯]
             collisions at sqrt[s]=1960  GeV recorded by the Collider
             Detector at Fermilab. No evidence for this state is found
             and an upper limit of 6.7% at the 95% confidence level is
             set on the fraction of B_{s}^{0} produced through the
             X(5568)→B_{s}^{0}π^{±} process.},
   Doi = {10.1103/physrevlett.120.202006},
   Key = {fds356687}
}

@article{fds308006,
   Author = {Collaboration, DAEACDF},
   Title = {Search for the flavor-changing neutral current decay
             D0-->µ+µ- in pp-bar collisions at sqrt[s]=1.96 TeV},
   Journal = {Physical Review},
   Volume = {D68},
   Number = {19},
   Pages = {091101},
   Year = {2003},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.101.192002},
   Abstract = {We report on a search for the flavor-changing neutral
             current decay D0-->µ+µ- in pp-bar collisions at
             sqrt[s]=1.96 TeV using 65 pb-1 of data collected by the
             CDF II experiment at the Fermilab Tevatron Collider. A
             displaced-track trigger selects long-lived D0 candidates in
             the D0-->µ+µ- search channel, the kinematically similar
             D0--> pi + pi - channel used for normalization, the
             Cabibbo-favored D0-->K- pi + channel used to optimize the
             selection criteria in an unbiased manner, and their charge
             conjugates. Finding no signal events in the D0-->µ+µ-
             search window, we set an upper limit on the branching
             fractionB(D0-- >µ+µ-)},
   Doi = {10.1103/physrevlett.101.192002},
   Key = {fds308006}
}

@article{fds351089,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G},
   Title = {Search for the HH → bb¯ bb¯ process via vector-boson
             fusion production using proton-proton collisions at √s =
             13 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {7},
   Year = {2020},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2020)108},
   Abstract = {A search for Higgs boson pair production via vector-boson
             fusion (VBF) in the bb¯ bb¯ final state is carried out
             with the ATLAS experiment using 126 fb−1 of proton- proton
             collision data delivered at s = 13 TeV by the Large Hadron
             Collider. This search is sensitive to VBF production of
             additional heavy bosons that may decay into Higgs boson
             pairs, and in a non-resonant topology it can constrain the
             quartic coupling between the Higgs bosons and vector bosons.
             No significant excess relative to the Standard Model
             expectation is observed, and limits on the production
             cross-section are set at the 95% confidence level for a
             heavy scalar resonance in the context of an extended Higgs
             sector, and for non-resonant Higgs boson pair production.
             Interpretation in terms of the coupling between a Higgs
             boson pair and two vector bosons is also provided: coupling
             values normalised to the Standard Model expectation of κ2V<
             −0.76 and κ2V> 2.90 are excluded at the 95% confidence
             level in data. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP07(2020)108},
   Key = {fds351089}
}

@article{fds356541,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez
             Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {Search for the Higgs boson decays H → ee and
             H → eμ in pp collisions at s=13TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {801},
   Year = {2020},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.135148},
   Abstract = {Searches for the Higgs boson decays H→ee and H→eμ are
             performed using data corresponding to an integrated
             luminosity of 139fb−1 collected with the ATLAS detector in
             pp collisions at s=13 TeV at the LHC. No significant signals
             are observed, in agreement with the Standard Model
             expectation. For a Higgs boson mass of 125 GeV, the observed
             (expected) upper limit at the 95% confidence level on the
             branching fraction B(H→ee) is 3.6×10−4 (3.5×10−4)
             and on B(H→eμ) is 6.2×10−5 (5.9×10−5). These
             results represent improvements by factors of about five and
             six on the previous best limits on B(H→ee) and B(H→eμ)
             respectively.},
   Doi = {10.1016/j.physletb.2019.135148},
   Key = {fds356541}
}

@article{fds307688,
   Author = {Aaltonen, T and González, BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
             A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
             ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De Barbaro and P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F},
   Title = {Search for the Higgs boson in the all-hadronic final state
             using the full CDF data set},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {2},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP02(2013)004},
   Abstract = {This paper reports the result of a search for the standard
             model Higgs boson in events containing four reconstructed
             jets associated with quarks. For masses below 135 GeV/c 2,
             the Higgs boson decays to bottom-antibottom quark pairs are
             dominant and result primarily in two hadronic jets. An
             additional two jets can be produced in the hadronic decay of
             a W or Z boson produced in association with the Higgs boson,
             or from the incoming quarks that produced the Higgs boson
             through the vector-boson fusion process. The search is
             performed using a sample of √s=1.96 TeV proton-antiproton
             collisions corresponding to an integrated luminosity of 9.45
             fb-1 recorded by the CDF II detector. The data are in
             agreement with the background model and 95% credibility
             level upper limits on Higgs boson production are set as a
             function of the Higgs boson mass. The median expected
             (observed) limit for a 125 GeV/c 2 Higgs boson is 11.0 (9.0)
             times the predicted standard model rate. © 2013
             SISSA.},
   Doi = {10.1007/JHEP02(2013)004},
   Key = {fds307688}
}

@article{fds307740,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten,
             K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa,
             HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks,
             KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde,
             M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benitez Garcia and JA and Benjamin, DP and Benoit,
             M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth,
             JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana,
             S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
             J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C},
   Title = {Search for the Higgs boson in the H→WW(*)→ℓ(+)νℓ(-)ν
             decay channel in pp collisions at √s=7 TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {11},
   Pages = {111802},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.108.111802},
   Abstract = {A search for the Higgs boson has been performed in the
             H→WW(*)→ℓ(+)νℓ(-)ν[over ¯] channel (ℓ=e/μ)
             with an integrated luminosity of 2.05 fb(-1) of pp
             collisions at √s=7 TeV collected with the ATLAS detector
             at the Large Hadron Collider. No significant excess of
             events over the expected background is observed and limits
             on the Higgs boson production cross section are derived for
             a Higgs boson mass in the range 110 GeV<m(H)<300 GeV. The
             observations exclude the presence of a standard model Higgs
             boson with a mass 145<m(H)<206 GeV at 95% confidence
             level.},
   Doi = {10.1103/physrevlett.108.111802},
   Key = {fds307740}
}

@article{fds307830,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
             G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
             M and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius,
             C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG},
   Title = {Search for the Higgs boson in the H→WW→lνjj decay
             channel in pp collisions at √s=7 TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {107},
   Number = {23},
   Pages = {231801},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.107.231801},
   Abstract = {A search for a Higgs boson has been performed in the
             H→WW→ℓνjj channel in 1.04 fb(-1) of pp collision data
             at √s=7 TeV recorded with the ATLAS detector at the Large
             Hadron Collider. No significant excess of events is observed
             over the expected background and limits on the Higgs boson
             production cross section are derived for a Higgs boson mass
             in the range 240 GeV<m(H)<600 GeV. The best sensitivity is
             reached for m(H)=400 GeV, where the 95% confidence level
             upper bound on the cross section for H→WW production is
             3.1 pb, or 2.7 times the standard model prediction.},
   Doi = {10.1103/physrevlett.107.231801},
   Key = {fds307830}
}

@article{fds307656,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Search for the Higgs boson in the H→WW→ℓνjj decay
             channel at √s=7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {718},
   Number = {2},
   Pages = {391-410},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {December},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.10.066},
   Abstract = {A search for the Standard Model Higgs boson has been
             performed in the H→WW→ℓνjj channel using 4.7 fb−1
             of pp collision data recorded at a centre-of-mass energy of
             s=7 TeV with the ATLAS detector at the Large Hadron
             Collider. Higgs boson candidates produced in association
             with zero, one or two jets are included in the analysis to
             maximize the acceptance for both gluon fusion and weak boson
             fusion Higgs boson production processes. No significant
             excess of events is observed over the expected background
             and limits on the Higgs boson production cross section are
             derived for a Higgs boson mass in the range 300 GeV<mH<600
             GeV. The best sensitivity is reached for mH=400 GeV, where
             the observed (expected) 95% confidence level upper bound on
             the cross section for H→WW produced in association with
             zero or one jet is 2.2 pb (1.9 pb), corresponding to 1.9
             (1.6) times the Standard Model prediction. In the Higgs
             boson plus two jets channel, which is more sensitive to the
             weak boson fusion process, the observed (expected) 95%
             confidence level upper bound on the cross section for H→WW
             production with mH=400 GeV is 0.7 pb (0.6 pb), corresponding
             to 7.9 (6.5) times the Standard Model prediction.},
   Doi = {10.1016/j.physletb.2012.10.066},
   Key = {fds307656}
}

@article{fds356654,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Search for the Higgs boson produced in association with a
             vector boson and decaying into two spin-zero particles in
             the H → aa → 4b channel in pp collisions at √s=13 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {10},
   Year = {2018},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2018)031},
   Abstract = {A search for exotic decays of the Higgs boson into a pair of
             spin-zero particles, H → aa, where the a-boson decay sin
             to b-quarks promptly or with a mean proper lifetime cτa up
             to 6 mm and has a mass in the range of 20–60 GeV, is
             presented. The search is performed in events where the Higgs
             boson is produced in association with a W or Z boson, giving
             rise to a signature of one or two charged leptons (electrons
             or muons) and multiple jets from b-quark decays. The
             analysis is based on the dataset of proton-proton collisions
             at s=13 TeV recorded in 2015 and 2016 by the ATLAS detector
             at the CERN Large Hadron Collider, corresponding to an
             integrated luminosity of 36.1 fb−1. No significant excess
             of events above the Standard Model background prediction is
             observed, and 95% confidence-level upper limits are derived
             for the production cross-sections for pp → WH, ZH and
             their combination, times the branching ratio of the decay
             chain H → aa → 4b. For a-bosons which decay promptly,
             the upper limit on the combination of cross-sections for WH
             and ZH times the branching ratio of H → aa → 4b ranges
             from 3.0 pb for ma = 20 GeV to 1.3 pb for ma = 60 GeV,
             assuming that the ratio of WH to ZH cross-sections follows
             the Standard Model prediction. For a-bosons with longer
             proper lifetimes, the most stringent limits are 1.8 pb and
             0.68 pb, respectively, at cτa ∼ 0.4 mm.[Figure not
             available: see fulltext.].},
   Doi = {10.1007/JHEP10(2018)031},
   Key = {fds356654}
}

@article{fds323242,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli,
             A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich,
             LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A},
   Title = {Search for the Higgs boson produced in association with a W
             boson and decaying to four b-quarks via two spin-zero
             particles in pp collisions at 13 TeV with the ATLAS
             detector.},
   Journal = {Eur Phys J C Part Fields},
   Volume = {76},
   Number = {11},
   Pages = {605},
   Year = {2016},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4418-9},
   Abstract = {This paper presents a dedicated search for exotic decays of
             the Higgs boson to a pair of new spin-zero particles,
             [Formula: see text], where the particle a decays to b-quarks
             and has a mass in the range of 20-60 GeV. The search is
             performed in events where the Higgs boson is produced in
             association with a [Formula: see text] boson, giving rise to
             a signature of a lepton (electron or muon), missing
             transverse momentum, and multiple jets from b-quark decays.
             The analysis is based on the full dataset of pp collisions
             at [Formula: see text] recorded in 2015 by the ATLAS
             detector at the CERN Large Hadron Collider, corresponding to
             an integrated luminosity of 3.2 [Formula: see text]. No
             significant excess of events above the Standard Model
             prediction is observed, and a [Formula: see text]
             confidence-level upper limit is derived for the product of
             the production cross section for [Formula: see text] times
             the branching ratio for the decay [Formula: see text]. The
             upper limit ranges from 6.2 pb for an a-boson mass
             [Formula: see text] to 1.5 pb for [Formula: see
             text].},
   Doi = {10.1140/epjc/s10052-016-4418-9},
   Key = {fds323242}
}

@article{fds308004,
   Author = {Aaltonen, T and others},
   Title = {Search for the Higgs Boson Produced in Association with
             Z→ℓ+ℓ- in pp̅ Collisions at sqrt[s] =1.96
             TeV},
   Journal = {Physical Review Letters},
   Volume = {101},
   Number = {25},
   Pages = {251803},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.251803},
   Abstract = {We present a search for the Higgs boson in the process qq̅
             →ZH→ℓ+ℓ-bb̅ . The analysis uses an integrated
             luminosity of 1  fb-1 of pp̅ collisions produced at
             sqrt[s]=1.96  TeV and accumulated by the upgraded
             Collider Detector at Fermilab (CDF II). We employ artificial
             neural networks both to correct jets mismeasured in the
             calorimeter and to distinguish the signal kinematic
             distributions from those of the background. We see no
             evidence for Higgs boson production, and set 95% C.L. upper
             limits on σZHB(H→bb̅ ), ranging from 1.5 to 1.2 pb for a
             Higgs boson mass (mH) of 110 to 150  GeV/c2.},
   Doi = {10.1103/physrevlett.101.251803},
   Key = {fds308004}
}

@article{fds307992,
   Author = {Aaltonen, T and others},
   Title = {Search for the Higgs boson produced in association with
             Z→ℓ+ℓ- using the matrix element method at CDF
             II},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {7},
   Pages = {071101},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.071101},
   Abstract = {We present a search for associated production of the
             standard model Higgs boson and a Z boson where the Z boson
             decays to two leptons and the Higgs decays to a pair of b
             quarks in pp̅ collisions at the Fermilab Tevatron. We use
             event probabilities based on standard model matrix elements
             to construct a likelihood function of the Higgs content of
             the data sample. In a CDF data sample corresponding to an
             integrated luminosity of 2.7  fb-1 we see no evidence of
             a Higgs boson with a mass between 100  GeV/c2 and
             150  GeV/c2. We set 95% confidence level upper limits on
             the cross section for ZH production as a function of the
             Higgs boson mass mH; the limit is 8.2 times the standard
             model prediction at mH=115  GeV/c2.},
   Doi = {10.1103/PhysRevD.80.071101},
   Key = {fds307992}
}

@article{fds310354,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Djuvsland, JI and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Kucuk, H and Anisenkov,
             AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Search for the lepton flavor violating decay Z → eμ in pp
             collisions at √s = 8 TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.072010},
   Abstract = {The ATLAS detector at the Large Hadron Collider is used to
             search for the lepton flavor violating process Z → eμ in
             pp collisions using 20.3 fb-1 of data collected at √s = 8
             TeV. An enhancement in the eμ invariant mass spectrum is
             searched for at the Z-boson mass. The number of Z bosons
             produced in the data sample is estimated using events of
             similar topology, Z → ee and μμ, significantly reducing
             the systematic uncertainty in the measurement. There is no
             evidence of an enhancement at the Z-boson mass, resulting in
             an upper limit on the branching fraction, B(Z → 7.5 ×
             10.7 at the 95% confidence level.},
   Doi = {10.1103/PhysRevD.90.072010},
   Key = {fds310354}
}

@article{fds307977,
   Author = {Aaltonen, T and others},
   Title = {Search for the neutral current top quark decay t→Zc using
             the ratio of Z-boson+4  jets to W-boson+4  jets
             production},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {5},
   Pages = {052001},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.052001},
   Abstract = {We have used the Collider Detector at Fermilab (CDF-II) to
             search for the flavor-changing neutral-current (FCNC)
             top-quark decay t→Zc using a technique employing ratios of
             W and Z production, measured in pp̅ data corresponding to
             an integrated luminosity of 1.52  fb-1. The analysis
             uses a comparison of two decay chains, pp̅ →tt̅
             →WbWb→ℓνbjjb and pp̅ →tt̅ →ZcWb→ℓℓcjjb,
             to cancel systematic uncertainties in acceptance,
             efficiency, and luminosity. We validate the modeling of
             acceptance and efficiency for lepton identification over the
             multiyear data set using another ratio of W and Z
             production, in this case the observed ratio of inclusive
             production of W to Z bosons. To improve the discrimination
             against standard model backgrounds to top-quark decays, we
             calculate the top-quark mass for each event with two leptons
             and four jets assuming it is a tt̅ event with one of the
             top quarks decaying to Zc. For additional background
             discrimination we require at least one jet to be identified
             as originating from a b quark. No significant signal is
             found and we set an upper limit on the FCNC branching ratio
             Br(t→Zc) using a likelihood constructed from the
             ℓℓcjjb top-quark mass distribution and the number of
             ℓνbjjb events. Limits are set as a function of the
             helicity of the Z boson produced in the FCNC decay. For 100%
             longitudinally-polarized Z bosons we find limits of 8.3% and
             9.3% (95% C.L.) depending on the assumptions regarding the
             theoretical top-quark pair production cross
             section.},
   Doi = {10.1103/PhysRevD.80.052001},
   Key = {fds307977}
}

@article{fds307630,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for the neutral Higgs bosons of the minimal
             supersymmetric standard model in pp collisions at √s = 7
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {2},
   Pages = {1-46},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP02(2013)095},
   Abstract = {A search for neutral Higgs bosons of the Minimal
             Supersymmetric Standard Model (MSSM) is reported. The
             analysis is based on a sample of proton-proton collisions at
             a centre-of-mass energy of 7TeV recorded with the ATLAS
             detector at the Large Hadron Collider. The data were
             recorded in 2011 and correspond to an integrated luminosity
             of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into
             oppositely-charged muon or τ lepton pairs are considered
             for final states requiring either the presence or absence of
             b-jets. No statistically significant excess over the
             expected background is observed and exclusion limits at the
             95% confidence level are derived. The exclusion limits are
             for the production cross-section of a generic neutral Higgs
             boson, φ, as a function of the Higgs boson mass and for
             h/A/H production in the MSSM as a function of the parameters
             mA and tan β in the mhmax scenario for mA in the range of
             90GeV to 500 GeV. Copyright CERN.},
   Doi = {10.1007/JHEP02(2013)095},
   Key = {fds307630}
}

@article{fds347444,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azoulay, AM and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines,
             JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi
             Gupta, D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee,
             S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
             G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous,
             S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall,
             A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
             A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary,
             O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertoli, G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bi, R and Bianchi,
             RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
             V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borecka-Bielska, HM and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau,
             JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner,
             R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
             PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch,
             TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
             H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carter, JWS and Casadei, D and Casado, MP and Casha,
             AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, WS and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen, H and Chen, J and Chen,
             S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng,
             HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont,
             AR and Chouridou, S},
   Title = {Search for the Production of a Long-Lived Neutral Particle
             Decaying within the ATLAS Hadronic Calorimeter in
             Association with a Z Boson from pp Collisions at
             sqrt[s]=13  TeV.},
   Journal = {Physical review letters},
   Volume = {122},
   Number = {15},
   Pages = {151801},
   Year = {2019},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.122.151801},
   Abstract = {This Letter presents a search for the production of a
             long-lived neutral particle (Z_{d}) decaying within the
             ATLAS hadronic calorimeter, in association with a standard
             model (SM) Z boson produced via an intermediate scalar
             boson, where Z→ℓ^{+}ℓ^{-} (ℓ=e, μ). The data used
             were collected by the ATLAS detector during 2015 and 2016 pp
             collisions with a center-of-mass energy of
             sqrt[s]=13  TeV at the Large Hadron Collider and
             correspond to an integrated luminosity of
             36.1±0.8  fb^{-1}. No significant excess of events is
             observed above the expected background. Limits on the
             production cross section of the scalar boson times its decay
             branching fraction into the long-lived neutral particle are
             derived as a function of the mass of the intermediate scalar
             boson, the mass of the long-lived neutral particle, and its
             cτ from a few centimeters to one hundred meters. In the
             case that the intermediate scalar boson is the SM Higgs
             boson, its decay branching fraction to a long-lived neutral
             particle with a cτ approximately between 0.1 and 7 m is
             excluded with a 95% confidence level up to 10% for
             m_{Z_{d}} between 5 and 15 GeV.},
   Doi = {10.1103/physrevlett.122.151801},
   Key = {fds347444}
}

@article{fds307947,
   Author = {Aaltonen, T and others},
   Title = {Search for the Production of Narrow tb̅ Resonances in 1.9
             fb-1 of pp̅ Collisions at sqrt[s] =1.96
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {4},
   Pages = {041801},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.041801},
   Abstract = {We present new limits on resonant tb̅ production in pp̅
             collisions at sqrt[s]=1.96  TeV, using 1.9  fb-1 of
             data recorded with the CDF II detector at the Fermilab
             Tevatron. We reconstruct a candidate tb̅ mass in events
             with a lepton, neutrino candidate, and two or three jets,
             and search for anomalous tb̅ production as modeled by
             W′→tb̅ . We set a new limit on a right-handed W′ with
             standard model-like coupling, excluding any mass below
             800  GeV/c2 at 95% C.L. The cross section for any
             narrow, resonant tb̅ production between 750 and
             950  GeV/c2 is found to be less than 0.28 pb at 95% C.L.
             We also present an exclusion of the W′ coupling strength
             versus W′ mass over the range 300--950  GeV/c2.},
   Doi = {10.1103/physrevlett.103.041801},
   Key = {fds307947}
}

@article{fds307899,
   Author = {Aaltonen, and T, and others},
   Title = {Search for the Production of Scalar Bottom Quarks in $p
             \bar{p}$ collisions at $\sqrt{s} = 1.96$
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {8},
   Pages = {081802},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.081802},
   Abstract = {http://arxiv.org/abs/1005.3600},
   Doi = {10.1103/PhysRevLett.105.081802},
   Key = {fds307899}
}

@article{fds314797,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for the production of single vector-like and excited
             quarks in the Wt final state in pp collisions at √s = 8
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {2},
   Pages = {1-46},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP02(2016)110},
   Abstract = {A search for vector-like quarks and excited quarks in events
             containing a top quark and a W boson in the final state is
             reported here. The search is based on 20.3 fb−1 of
             proton-proton collision data taken at the LHC at a
             centre-of-mass energy of 8 TeV recorded by the ATLAS
             detector. Events with one or two leptons, and one, two or
             three jets are selected with the additional requirement that
             at least one jet contains a b-quark. Single-lepton events
             are also required to contain at least one large-radius jet
             from the hadronic decay of a high-pTW boson or a top quark.
             No significant excess over the expected background is
             observed and upper limits on the cross-section times
             branching ratio for different vector-like quark and
             excited-quark model masses are derived. For the
             excited-quark production and decay to Wt with unit
             couplings, quarks with masses below 1500 GeV are excluded
             and coupling-dependent limits are set.},
   Doi = {10.1007/JHEP02(2016)110},
   Key = {fds314797}
}

@article{fds307562,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Search for the production of ZW and ZZ boson pairs decaying
             into charged leptons and jets in pp̄ collisions at
             √s=1.96 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {9},
   Pages = {092002},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.092002},
   Abstract = {We present a measurement of the production cross section for
             ZW and ZZ boson pairs in final states with a pair of charged
             leptons, from the decay of a Z boson, and at least two jets,
             from the decay of a W or Z boson, using the full sample of
             proton-antiproton collisions recorded with the CDF II
             detector at the Tevatron, corresponding to 8.9 fb-1 of
             integrated luminosity. We increase the sensitivity to
             vector-boson decays into pairs of quarks using a
             neural-network discriminant that exploits the differences
             between the spatial spread of energy depositions and
             charged-particle momenta contained within the jet of
             particles originating from quarks and gluons. Additionally,
             we employ new jet energy corrections to Monte Carlo
             simulations that account for differences in the observed
             energy scales for quark and gluon jets. The number of signal
             events is extracted through a simultaneous fit to the dijet
             mass spectrum in three classes of events: events likely to
             contain jets with a heavy-quark decay, events likely to
             contain jets originating from light quarks, and events that
             fail these identification criteria. We determine the
             production cross section to be σZW+ZZ=2.5-1.0+2.0 pb (<6.1
             pb at the 95% confidence level), consistent with the
             standard model prediction of 5.1 pb. © 2013 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.88.092002},
   Key = {fds307562}
}

@article{fds307969,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
             F and Bednar, P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
             A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
             A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli,
             M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi,
             R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G},
   Title = {Search for the rare decays B+→μ+μ-K+, B0→μ+μ-
             K*(892)0, and Bs0→μ+μ- at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.011104},
   Abstract = {We search for b→sμ+μ- transitions in B meson (B+, B0, or
             Bs0) decays with 924pb-1 of pp̄ collisions at s=1.96TeV
             collected with the CDF II detector at the Fermilab Tevatron.
             We find excesses with significances of 4.5, 2.9, and 2.4
             standard deviations in the B+→μ+μ-K+,
             B0→μ+μ-K*(892)0, and Bs0→μ+μ- decay modes,
             respectively. Using B→J/ψh (h=K+, K*(892)0,) decays as
             normalization channels, we report branching fractions for
             the previously observed B+ and B0 decays,
             B(B+→μ+μ-K+)=(0.59±0.15±0. 04)×10-6, and
             B(B0→μ+μ-K*(892)0)=(0.81±0. 30±0.10)×10-6, where the
             first uncertainty is statistical, and the second is
             systematic. We set an upper limit on the relative branching
             fraction B(Bs0→μ+μ-)/B(Bs0→J/ψ)<2.6(2.3)×10-3 at the
             95(90)% confidence level, which is the most stringent to
             date. © 2009 The American Physical Society.},
   Doi = {10.1103/PhysRevD.79.011104},
   Key = {fds307969}
}

@article{fds307805,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R},
   Title = {Search for the rare radiative decay W→πγ in pp̄
             collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.032001},
   Abstract = {We present a search for the rare radiative decay W ±→ π
             ±γ using data corresponding to an integrated luminosity of
             4.3fb -1 of proton-antiproton collisions at a center-of-mass
             energy of 1.96 TeV collected by the CDF experiment at
             Fermilab. As no statistically significant signal is
             observed, we set a 95%-confidence-level upper limit on the
             relative branching fraction Γ(W ±→π ±γ)/Γ(W ±→e
             ±ν) at 6.4×10 -5, a factor of 10 improvement over the
             previous limit. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.85.032001},
   Key = {fds307805}
}

@article{fds308175,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin,
             B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto,
             J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette,
             F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar,
             V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
             F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR},
   Title = {Search for the Scalar Top Quark in [Formula presented]
             Collisions at [Formula presented]},
   Journal = {Physical Review Letters},
   Volume = {88},
   Number = {17},
   Pages = {6},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.88.171802},
   Abstract = {We have performed a search for scalar top quark (stop) pair
             production in the inclusive electron-muon-missing transverse
             energy final state, using a sample of [Formula presented]
             events corresponding to [Formula presented] of data
             collected with the D0 detector at Fermilab. The search is
             done in the framework of the minimal supersymmetric standard
             model assuming that the sneutrino is the lightest
             supersymmetric particle. For the dominant decays of the
             lightest stop, [Formula presented] and [Formula presented],
             no evidence for signal is found. We derive cross-section
             limits as a function of stop ([Formula presented]), chargino
             ([Formula presented]), and sneutrino ([Formula presented])
             masses. © 2002 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.88.171802},
   Key = {fds308175}
}

@article{fds310382,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for the Standard Model Higgs boson decay to
             μ+μ with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {738},
   Number = {1},
   Pages = {68-86},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.09.008},
   Abstract = {A search is reported for Higgs boson decay to μ+μ− using
             data with an integrated luminosity of 24.8 fb−1collected
             with the ATLAS detector in pp collisions at s=7and8 TeV at
             the CERN Large Hadron Collider. The observed dimuon
             invariant mass distribution is consistent with the Standard
             Model background-only hypothesis in the 120–150 GeV search
             range. For a Higgs boson with a mass of 125.5 GeV, the
             observed (expected) upper limit at the 95% confidence level
             is 7.0 (7.2) times the Standard Model expectation. This
             corresponds to an upper limit on the branching ratio
             BR(H→μ+μ−) of 1.5×10−3.},
   Doi = {10.1016/j.physletb.2014.09.008},
   Key = {fds310382}
}

@article{fds317296,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Search for the Standard Model Higgs boson decaying into bb¯
             produced in association with top quarks decaying
             hadronically in pp collisions at √s = 8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2016)160},
   Abstract = {A search for Higgs boson production in association with a
             pair of top quarks (tt¯ H) is performed, where the Higgs
             boson decays to bb¯, and both top quarks decay
             hadronically. The data used correspond to an integrated
             luminosity of 20.3 fb−1 of pp collisions at √s = 8 TeV
             collected with the ATLAS detector at the Large Hadron
             Collider. The search selects events with at least six
             energetic jets and uses a boosted decision tree algorithm to
             discriminate between signal and Standard Model background.
             The dominant multijet background is estimated using a
             dedicated data-driven technique. For a Higgs boson mass of
             125 GeV, an upper limit of 6.4 (5.4) times the Standard
             Model cross section is observed (expected) at 95% confidence
             level. The best-fit value for the signal strength is μ =
             1.6 ± 2.6 times the Standard Model expectation for mH = 125
             GeV. Combining all tt¯ H searches carried out by ATLAS at
             √s = 8 and 7 TeV, an observed (expected) upper limit of
             3.1 (1.4) times the Standard Model expectation is obtained
             at 95% confidence level, with a signal strength μ = 1.7 ±
             0.8.},
   Doi = {10.1007/JHEP05(2016)160},
   Key = {fds317296}
}

@article{fds307686,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
             ME and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci,
             A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
             A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
             ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
             P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington,
             S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest,
             R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic,
             I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Search for the standard model Higgs boson decaying to a bb
             pair in events with no charged leptons and large missing
             transverse energy using the full CDF data
             set.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {11},
   Pages = {111805},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevlett.109.111805},
   Abstract = {We report on a search for the standard model Higgs boson
             produced in association with a vector boson in the full data
             set of proton-antiproton collisions at sqrt[s]=1.96  TeV
             recorded by the CDF II detector at the Tevatron,
             corresponding to an integrated luminosity of
             9.45  fb(-1). We consider events having no identified
             charged lepton, a transverse energy imbalance, and two or
             three jets, of which at least one is consistent with
             originating from the decay of a b quark. We place 95%
             credibility level upper limits on the production cross
             section times standard model branching fraction for several
             mass hypotheses between 90 and 150  GeV/c(2). For a
             Higgs boson mass of 125  GeV/c(2), the observed
             (expected) limit is 6.7 (3.6) times the standard model
             prediction.},
   Doi = {10.1103/physrevlett.109.111805},
   Key = {fds307686}
}

@article{fds307775,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak,
             MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber,
             T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz,
             SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
             Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada,
             LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini,
             I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro,
             NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung,
             SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland,
             W},
   Title = {Search for the Standard Model Higgs boson in the decay
             channel H→ZZ(*)→4ℓ with 4.8 fb-1
             of pp collision data at √s=7 TeV with ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {710},
   Number = {3},
   Pages = {383-402},
   Publisher = {Elsevier BV},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.03.005},
   Abstract = {This Letter presents a search for the Standard Model Higgs
             boson in the decay channel H→ZZ(*)→ℓ+ℓ-ℓ'+ℓ'-,
             where ℓ, ℓ'=e or μ, using proton-proton collisions at
             √s=7 TeV recorded with the ATLAS detector and
             corresponding to an integrated luminosity of 4.8 fb-1. The
             four-lepton invariant mass distribution is compared with
             Standard Model background expectations to derive upper
             limits on the cross section of a Standard Model Higgs boson
             with a mass between 110 GeV and 600 GeV. The mass ranges
             134-156 GeV, 182-233 GeV, 256-265 GeV and 268-415 GeV are
             excluded at the 95% confidence level. The largest upward
             deviations from the background-only hypothesis are observed
             for Higgs boson masses of 125 GeV, 244 GeV and 500 GeV with
             local significances of 2.1, 2.2 and 2.1 standard deviations,
             respectively. Once the look-elsewhere effect is considered,
             none of these excesses are significant. © 2012
             CERN.},
   Doi = {10.1016/j.physletb.2012.03.005},
   Key = {fds307775}
}

@article{fds307860,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for the Standard Model Higgs boson in the decay
             channel H→ZZ(*)→4ℓ with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {5},
   Pages = {435-451},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.10.034},
   Abstract = {A search for the Standard Model Higgs boson in the decay
             channel H→ZZ(*)→ℓ+ℓ-ℓ'+ℓ'-, where ℓ=e, μ, is
             presented. Proton-proton collision data at s=7TeV recorded
             with the ATLAS detector and corresponding to an average
             integrated luminosity of 2.1fb-1 are compared to the
             Standard Model expectations. Upper limits on the production
             cross section of a Standard Model Higgs boson with a mass
             between 110 and 600GeV are derived. The observed (expected)
             95% confidence level upper limit on the production cross
             section for a Higgs boson with a mass of 194 GeV, the region
             with the best expected sensitivity for this search, is 0.99
             (1.01) times the Standard Model prediction. The Standard
             Model Higgs boson is excluded at 95% confidence level in the
             mass ranges 191-197, 199-200 and 214-224 GeV. © 2011
             CERN.},
   Doi = {10.1016/j.physletb.2011.10.034},
   Key = {fds307860}
}

@article{fds307711,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni,
             G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth,
             CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC},
   Title = {Search for the standard model Higgs boson in the diphoton
             decay channel with 4.9 fb(-1) of pp collision data at √s=7
             TeV with ATLAS.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {11},
   Pages = {111803},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.108.111803},
   Abstract = {A search for the standard model Higgs boson is performed in
             the diphoton decay channel. The data used correspond to an
             integrated luminosity of 4.9 fb(-1) collected with the ATLAS
             detector at the Large Hadron Collider in proton-proton
             collisions at a center-of-mass energy of √s=7 TeV. In the
             diphoton mass range 110-150 GeV, the largest excess with
             respect to the background-only hypothesis is observed at
             126.5 GeV, with a local significance of 2.8 standard
             deviations. Taking the look-elsewhere effect into account in
             the range 110-150 GeV, this significance becomes 1.5
             standard deviations. The standard model Higgs boson is
             excluded at 95% confidence level in the mass ranges of
             113-115 GeV and 134.5-136 GeV.},
   Doi = {10.1103/physrevlett.108.111803},
   Key = {fds307711}
}

@article{fds307788,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Arfaoui, S and Arguin J-F., and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
             A and Artoni, G},
   Title = {Search for the Standard Model Higgs boson in the H →
             τ+τ- decay mode in √s = 7TeV pp
             collisions with ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP09(2012)070},
   Abstract = {A search for the Standard Model Higgs boson decaying into a
             pair of τ leptons is reported. The analysis is based on a
             data sample of proton-proton collisions collected by the
             ATLAS experiment at the LHC and corresponding to an
             integrated luminosity of 4.7fb-1. No significant excess over
             the expected background is observed in the Higgs boson mass
             range of 100-150 GeV. The observed (expected) upper limits
             on the cross section times the branching ratio for H →
             τ+τ- are found to be between 2.9 (3.4) and 11.7 (8.2)
             times the Standard Model prediction for this mass
             range.},
   Doi = {10.1007/JHEP09(2012)070},
   Key = {fds307788}
}

@article{fds313623,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel,
             M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
             M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
             T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins,
             NJ and Collins-Tooth, C and Collot, J},
   Title = {Search for the Standard Model Higgs boson in the
             H→WW({star operator})→ℓνℓν decay mode
             with 4.7 fb-1 of ATLAS data at √s=7
             TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {716},
   Number = {1},
   Pages = {62-81},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.08.010},
   Abstract = {A search for the Standard Model Higgs boson in the
             H→WW({star operator})→ℓνℓν (ℓ=e, μ) decay mode
             is presented. The search is performed using proton-proton
             collision data corresponding to an integrated luminosity of
             4.7 fb-1 at a centre-of-mass energy of 7 TeV collected
             during 2011 with the ATLAS detector at the Large Hadron
             Collider. No significant excess of events over the expected
             background is observed. An upper bound is placed on the
             Higgs boson production cross section as a function of its
             mass. A Standard Model Higgs boson with mass in the range
             between 133 GeV and 261 GeV is excluded at 95% confidence
             level, while the expected exclusion range is from 127 GeV to
             233 GeV. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.08.010},
   Key = {fds313623}
}

@article{fds307859,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for the Standard Model Higgs boson in the two photon
             decay channel with the ATLAS detector at the
             LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {5},
   Pages = {452-470},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.10.051},
   Abstract = {A search for the Standard Model Higgs boson in the two
             photon decay channel is reported, using 1.08 fb-1 of
             proton-proton collision data at a centre-of-mass energy of 7
             TeV recorded by the ATLAS detector. No significant excess is
             observed in the investigated mass range of 110-150 GeV.
             Upper limits on the cross-section times branching ratio of
             between 2.0 and 5.8 times the Standard Model prediction are
             derived for this mass range. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.10.051},
   Key = {fds307859}
}

@article{fds321078,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
   Title = {Search for the Standard Model Higgs boson produced by
             vector-boson fusion and decaying to bottom quarks in √s=8
             TeV pp collisions with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2016)112},
   Abstract = {A search with the ATLAS detector is presented for the
             Standard Model Higgs boson produced by vector-boson fusion
             and decaying to a pair of bottom quarks, using 20.2 fb−1
             of LHC proton-proton collision data at s=8 TeV. The signal
             is searched for as a resonance in the invariant mass
             distribution of a pair of jets containing b-hadrons in
             vector-boson-fusion candidate events. The yield is measured
             to be −0.8 ± 2.3 times the Standard Model cross-section
             for a Higgs boson mass of 125 GeV. The upper limit on the
             cross-section times the branching ratio is found to be 4.4
             times the Standard Model cross-section at the 95% confidence
             level, consistent with the expected limit value of 5.4 (5.7)
             in the background-only (Standard Model production)
             hypothesis.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP11(2016)112},
   Key = {fds321078}
}

@article{fds316850,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for the standard model Higgs boson produced in
             association with a vector boson and decaying into a tau pair
             in pp collisions at s =8 TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {93},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {May},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.092005},
   Abstract = {A search for the standard model Higgs boson produced in
             association with a vector boson with the decay H→ττ is
             presented. The data correspond to 20.3 fb-1 of integrated
             luminosity from proton-proton collisions at s=8 TeV recorded
             by the ATLAS experiment at the LHC during 2012. The data
             agree with the background expectation, and 95%
             confidence-level upper limits are placed on the cross
             section of this process. The observed (expected) limit,
             expressed in terms of the signal strength μ=σ/σSM for
             mH=125 GeV, is μ<5.6 (3.7). The measured value of the
             signal strength is μ=2.3±1.6.},
   Doi = {10.1103/PhysRevD.93.092005},
   Key = {fds316850}
}

@article{fds307657,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             TJ and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amonm, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeenm, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Anger, R and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber,
             T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, R and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, R and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Bege,
             M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, R and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botteri, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido,
             MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casadoll, MP and Cascela,
             M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Catastini, R and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavalleri, R and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RI and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, TJ and Cogneras, E and Colas, J and Colijn, AP and Collins,
             NJ and Collins-Tooth, C},
   Title = {Search for the Standard Model Higgs boson produced in
             association with a vector boson and decaying to a
             b-quark pair with the ATLAS detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {718},
   Number = {2},
   Pages = {369-390},
   Publisher = {Elsevier BV},
   Year = {2012},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.10.061},
   Abstract = {© 2012 CERN This Letter presents the results of a direct
             search with the ATLAS detector at the LHC for a Standard
             Model Higgs boson of mass 110⩽mH⩽130 GeV produced in
             association with a W or Z boson and decaying to bb¯. Three
             decay channels are considered: ZH→ℓ+ℓ−bb¯
             WH→ℓνbb¯ and ZH→νν¯bb¯ where ℓ corresponds to
             an electron or a muon. No evidence for Higgs boson
             production is observed in a dataset of 7 TeV pp collisions
             corresponding to 4.7 fb−1 of integrated luminosity
             collected by ATLAS in 2011. Exclusion limits on Higgs boson
             production, at the 95% confidence level, of 2.5 to 5.5 times
             the Standard Model cross section are obtained in the mass
             range 110–130 GeV. The expected exclusion limits range
             between 2.5 and 4.9 for the same mass interval.},
   Doi = {10.1016/j.physletb.2012.10.061},
   Key = {fds307657}
}

@article{fds307819,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'errico, M},
   Title = {Search for the standard model Higgs boson produced in
             association with a W ± boson with 7.5fb
             -1 integrated luminosity at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.032011},
   Abstract = {We present a search for the standard model Higgs boson
             produced in association with a W ± boson. This search uses
             data corresponding to an integrated luminosity of 7.5fb -1
             collected by the CDF detector at the Tevatron. We select
             WH→νbb̄ candidate events with two jets, large missing
             transverse energy, and exactly one charged lepton. We
             further require that at least one jet be identified to
             originate from a bottom quark. Discrimination between the
             signal and the large background is achieved through the use
             of a Bayesian artificial neural network. The number of
             tagged events and their distributions are consistent with
             the standard model expectations. We observe no evidence for
             a Higgs boson signal and set 95% C.L. upper limits on the WH
             production cross section times the branching ratio to decay
             to bb̄ pairs, σ(pp̄→W ±H) ×B(H→bb̄), relative to
             the rate predicted by the standard model. For the Higgs
             boson mass range of 100 to 150GeV/c2 we set observed
             (expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For
             115GeV/c2 the upper limit is 3.64 (2.78). The combination of
             the present search with an independent analysis that selects
             events with three jets yields more stringent limits ranging
             from 1.12 (1.79) to 34.4 (21.6) in the same mass range. For
             115 and 125GeV/c2 the upper limits are 2.65 (2.60) and 4.36
             (3.69), respectively. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.86.032011},
   Key = {fds307819}
}

@article{fds307821,
   Author = {Kotwal, AV and Collaboration, CDF},
   Title = {Search for the standard model Higgs boson produced in
             association with a Z boson in 7.9/fb of ppbar collisions at
             sqrt(s)=1.96 TeV using the CDF II detector},
   Journal = {Phys. Lett. B},
   Volume = {715},
   Number = {1-3},
   Pages = {98},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.07.045},
   Abstract = {We present a search for the standard model Higgs boson
             produced in association with a Z boson, using up to 7.9 fb
             -1 of integrated luminosity from pp- collisions collected
             with the CDF II detector. We utilize several novel
             techniques, including multivariate lepton selection,
             multivariate trigger parametrization, and a multi-stage
             signal discriminant consisting of specialized functions
             trained to distinguish individual backgrounds. By increasing
             acceptance and enhancing signal discrimination, these
             techniques have significantly improved the sensitivity of
             the analysis above what was expected from a larger dataset
             alone. We observe no significant evidence for a signal, and
             we set limits on the ZH production cross section. For a
             Higgs boson with mass 115 GeV/c 2, we expect (observe) a
             limit of 3.9 (4.8) times the standard model predicted value,
             at the 95% credibility level. © 2012 Elsevier
             B.V.},
   Doi = {10.1016/j.physletb.2012.07.045},
   Key = {fds307821}
}

@article{fds356690,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
             F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
             MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
             M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
             JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez,
             O and Arnold, H and Arratia, M},
   Title = {Search for the standard model Higgs boson produced in
             association with top quarks and decaying into a bb¯ pair in
             pp collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {97},
   Number = {7},
   Year = {2018},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.97.072016},
   Abstract = {A search for the standard model Higgs boson produced in
             association with a top-quark pair, ttH, is presented. The
             analysis uses 36.1 fb-1 of pp collision data at s=13 TeV
             collected with the ATLAS detector at the Large Hadron
             Collider in 2015 and 2016. The search targets the H→bb
             decay mode. The selected events contain either one or two
             electrons or muons from the top-quark decays, and are then
             categorized according to the number of jets and how likely
             these are to contain b-hadrons. Multivariate techniques are
             used to discriminate between signal and background events,
             the latter being dominated by tt+jets production. For a
             Higgs boson mass of 125 GeV, the ratio of the measured ttH
             signal cross-section to the standard model expectation is
             found to be μ=0.84-0.61+0.64. A value of μ greater than
             2.0 is excluded at 95% confidence level (C.L.) while the
             expected upper limit is μ<1.2 in the absence of a ttH
             signal.},
   Doi = {10.1103/PhysRevD.97.072016},
   Key = {fds356690}
}

@article{fds310331,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Piqueras, DÁ and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
             C},
   Title = {Search for the Standard Model Higgs boson produced in
             association with top quarks and decaying into [Formula: see
             text] in [Formula: see text] collisions at [Formula: see
             text] with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {349},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3543-1},
   Abstract = {A search for the Standard Model Higgs boson produced in
             association with a top-quark pair, [Formula: see text], is
             presented. The analysis uses 20.3 fb<sup>-1</sup> of
             <i>pp</i> collision data at [Formula: see text], collected
             with the ATLAS detector at the Large Hadron Collider during
             2012. The search is designed for the [Formula: see text]
             decay mode and uses events containing one or two electrons
             or muons. In order to improve the sensitivity of the search,
             events are categorised according to their jet and
             <i>b</i>-tagged jet multiplicities. A neural network is used
             to discriminate between signal and background events, the
             latter being dominated by [Formula: see text]+jets
             production. In the single-lepton channel, variables
             calculated using a matrix element method are included as
             inputs to the neural network to improve discrimination of
             the irreducible [Formula: see text] background. No
             significant excess of events above the background
             expectation is found and an observed (expected) limit of 3.4
             (2.2) times the Standard Model cross section is obtained at
             95 % confidence level. The ratio of the measured [Formula:
             see text] signal cross section to the Standard Model
             expectation is found to be [Formula: see text] assuming a
             Higgs boson mass of 125[Formula: see text].},
   Doi = {10.1140/epjc/s10052-015-3543-1},
   Key = {fds310331}
}

@article{fds310311,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for the Xb and other hidden-beauty states
             in the π+πϒ(1S) channel at
             ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {740},
   Pages = {199-217},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.11.055},
   Abstract = {This Letter presents a search for a hidden-beauty
             counterpart of the X(3872) in the mass ranges of
             10.05–10.31 GeV and 10.40–11.00 GeV, in the channel
             Xb→π+π−ϒ(1S)(→μ+μ−), using 16.2 fb−1 of s=8
             TeV pp collision data collected by the ATLAS detector at the
             LHC. No evidence for new narrow states is found, and upper
             limits are set on the product of the Xb cross section and
             branching fraction, relative to those of the ϒ(2S), at the
             95% confidence level using the CLS approach. These limits
             range from 0.8% to 4.0%, depending on mass. For masses above
             10.1 GeV, the expected upper limits from this analysis are
             the most restrictive to date. Searches for production of the
             ϒ(13DJ), ϒ(10860), and ϒ(11020) states also reveal no
             significant signals.},
   Doi = {10.1016/j.physletb.2014.11.055},
   Key = {fds310311}
}

@article{fds376063,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye,
             T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal,
             A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja,
             S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh,
             B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
             SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
             CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L},
   Title = {Search for the Zγ decay mode of new high-mass resonances in
             pp collisions at s=13 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {848},
   Year = {2024},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2023.138394},
   Abstract = {This letter presents a search for narrow, high-mass
             resonances in the Zγ final state with the Z boson decaying
             into a pair of electrons or muons. The s=13 TeV pp collision
             data were recorded by the ATLAS detector at the CERN Large
             Hadron Collider and have an integrated luminosity of 140
             fb−1. The data are found to be in agreement with the
             Standard Model background expectation. Upper limits are set
             on the resonance production cross section times the decay
             branching ratio into Zγ. For spin-0 resonances produced via
             gluon–gluon fusion, the observed limits at 95% confidence
             level vary between 65.5 fb and 0.6 fb, while for spin-2
             resonances produced via gluon–gluon fusion (or
             quark–antiquark initial states) limits vary between 77.4
             (76.1) fb and 0.6 (0.5) fb, for the mass range from 220 GeV
             to 3400 GeV.},
   Doi = {10.1016/j.physletb.2023.138394},
   Key = {fds376063}
}

@article{fds307887,
   Author = {Aaltonen, TEA},
   Title = {Search for the {H}iggs boson in the all-hadronic final state
             using the {CDF II} detector},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {5},
   Pages = {052010},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.052010},
   Abstract = {We report on a search for the production of the Higgs boson
             decaying to two bottom quarks accompanied by two additional
             quarks. The data sample used corresponds to an integrated
             luminosity of approximately 4fb-1 of pp̄ collisions at
             √s=1.96TeV recorded by the CDF II experiment. This search
             includes twice the integrated luminosity of the previous
             published result, uses analysis techniques to distinguish
             jets originating from light flavor quarks and those from
             gluon radiation, and adds sensitivity to a Higgs boson
             produced by vector boson fusion. We find no evidence of the
             Higgs boson and place limits on the Higgs boson production
             cross section for Higgs boson masses between 100GeV/c2 and
             150GeV/c2 at the 95% confidence level. For a Higgs boson
             mass of 120GeV/c2, the observed (expected) limit is 10.5
             (20.0) times the predicted standard model cross section. ©
             2011 American Physical Society.},
   Doi = {10.1103/PhysRevD.84.052010},
   Key = {fds307887}
}

@article{fds307651,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
             VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
   Title = {Search for third generation scalar leptoquarks in pp
             collisions at √s=7 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP06(2013)033},
   Abstract = {A search for pair-produced third generation scalar
             leptoquarks is presented, using proton-proton collisions at
             s=7 TeV at the LHC. The data were recorded with the ATLAS
             detector and correspond to an integrated luminosity of 4.7
             fb-1. Each leptoquark is assumed to decay to a tau lepton
             and a b-quark with a branching fraction equal to 100%. No
             statistically significant excess above the Standard Model
             expectation is observed. Third generation leptoquarks are
             therefore excluded at 95% confidence level for masses less
             than 534GeV. [Figure not available: see fulltext.] © 2013
             Cern for the benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP06(2013)033},
   Key = {fds307651}
}

@article{fds307684,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for top and bottom squarks from gluino pair
             production in final states with missing transverse energy
             and at least three b-jets with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2174-z},
   Abstract = {This letter reports the results of a search for top and
             bottom squarks from gluino pair production in 4.7 fb−1of
             pp collisions at √s = 7 TeV using the ATLAS detector at
             the LHC. The search is performed in events with large
             missing transverse momentum and at least three jets
             identified as originating from a b-quark. Exclusion limits
             are presented for a variety of gluino-mediated models with
             gluino masses up to 1 TeV excluded.},
   Doi = {10.1140/epjc/s10052-012-2174-z},
   Key = {fds307684}
}

@article{fds313585,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O},
   Title = {Search for top quark decays t → qH with H → γγ using
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {6},
   Year = {2014},
   Month = {January},
   ISSN = {1126-6708},
   url = {http://dx.doi.org/10.1007/JHEP06(2014)008},
   Abstract = {A search is performed for flavour-changing neutral currents
             in the decay of a top quark to an up-type (c, u) quark and a
             Higgs boson, where the Higgs boson decays to two photons.
             The proton-proton collision data set used corresponds to 4.7
             fb-1 at √ = 7TeV and 20.3fb-1 at √ = 8TeV collected by
             the ATLAS experiment at the LHC. Top quark pair events are
             searched for in which one top quark decays to qH and the
             other decays to bW. Both the hadronic and the leptonic decay
             modes of the W boson are used. No significant signal is
             observed and an upper limit is set on the t → qH branching
             ratio of 0.79 at the 95% confidence level. The corresponding
             limit on the tqH coupling combination λtcH2 + λtuH2 is
             0.17. © 2014 The Author(s).},
   Doi = {10.1007/JHEP06(2014)008},
   Key = {fds313585}
}

@article{fds356732,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Search for top quark decays t → qH, with H → γγ, in
             √s=13 TeV pp collisions using the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {10},
   Year = {2017},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2017)129},
   Abstract = {This article presents a search for flavour-changing neutral
             currents in the decay of a top quark into an up-type (q = c,
             u) quark and a Higgs boson, where the Higgs boson decays
             into two photons. The proton-proton collision data set
             analysed amounts to 36.1 fb−1 at s=13 TeV collected by the
             ATLAS experiment at the LHC. Top quark pair events are
             searched for, where one top quark decays into qH and the
             other decays into bW. Both the hadronic and leptonic decay
             modes of the W boson are used. No significant excess is
             observed and an upper limit is set on the t → cH branching
             ratio of 2.2 × 10−3 at the 95% confidence level, while
             the expected limit in the absence of signal is 1.6 ×
             10−3. The corresponding limit on the tcH coupling is 0.090
             at the 95% confidence level. The observed upper limit on the
             t → uH branching ratio is 2.4 × 10−3.[Figure not
             available: see fulltext.].},
   Doi = {10.1007/JHEP10(2017)129},
   Key = {fds356732}
}

@article{fds310348,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for top squark pair production in final states with
             one isolated lepton, jets, and missing transverse momentum
             in √ s = 8 TeV pp collisions with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2014)118},
   Abstract = {The results of a search for top squark (stop) pair
             production in final states with one isolated lepton, jets,
             and missing transverse momentum are reported. The analysis
             is performed with proton-proton collision data at (Formula
             presented.) = 8 TeV collected with the ATLAS detector at the
             LHC in 2012 corresponding to an integrated luminosity of 20
             fb−1. The lightest supersymmetric particle (LSP) is taken
             to be the lightest neutralino which only interacts weakly
             and is assumed to be stable. The stop decay modes considered
             are those to a top quark and the LSP as well as to a bottom
             quark and the lightest chargino, where the chargino decays
             to the LSP by emitting a W boson. A wide range of scenarios
             with different mass splittings between the stop, the
             lightest neutralino and the lightest chargino are
             considered, including cases where the W bosons or the top
             quarks are off-shell. Decay modes involving the heavier
             charginos and neutralinos are addressed using a set of
             phenomenological models of supersymmetry. No significant
             excess over the Standard Model prediction is observed. A
             stop with a mass between 210 and 640 GeV decaying directly
             to a top quark and a massless LSP is excluded at 95%
             confidence level, and in models where the mass of the
             lightest chargino is twice that of the LSP, stops are
             excluded at 95% confidence level up to a mass of 500 GeV for
             an LSP mass in the range of 100 to 150 GeV. Stringent
             exclusion limits are also derived for all other stop decay
             modes considered, and model-independent upper limits are set
             on the visible cross-section for processes beyond the
             Standard Model.},
   Doi = {10.1007/JHEP11(2014)118},
   Key = {fds310348}
}

@booklet{Abachi98,
   Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Álvarez, G and Alves,
             GA and Amidi, E and Amos, N and Anderson, EW and Aronson, SH and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Bendich, J and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Bischoff, A and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt,
             A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty,
             D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
             C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and De,
             K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard,
             J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahey, S and Fahland, T and Fatyga, M and Fatyga, MK and Featherly, J and Feher, S},
   Title = {Search for top squark pair production in the dielectron
             channel},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {57},
   Number = {1},
   Pages = {589-593},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.57.589},
   Abstract = {This report describes the first search for top squark pair
             production in the channel (Formula presented)+jets+(Formula
             presented) using (Formula presented) pb(Formula presented)
             of data collected using the DØ detector. A 95% confidence
             level upper limit on (Formula presented) is presented. The
             limit is above the theoretical expectation for (Formula
             presented) for this process, but does show the sensitivity
             of the current DØ data set to a particular topology for new
             physics. © 1998 The American Physical Society.},
   Doi = {10.1103/PhysRevD.57.589},
   Key = {Abachi98}
}

@article{fds356673,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki,
             M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Arnaez, O and Arnold, H and Arratia, M},
   Title = {Search for top squarks decaying to tau sleptons in pp
             collisions at s =13 Te v with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {98},
   Number = {3},
   Year = {2018},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.98.032008},
   Abstract = {A search for direct pair production of top squarks in final
             states with two tau leptons, b-jets, and missing transverse
             momentum is presented. The analysis is based on
             proton-proton collision data at s=13 TeV corresponding to an
             integrated luminosity of 36.1 fb-1 recorded with the ATLAS
             detector at the Large Hadron Collider in 2015 and 2016. Two
             exclusive channels with either two hadronically decaying tau
             leptons or one hadronically and one leptonically decaying
             tau lepton are considered. No significant deviation from the
             Standard Model predictions is observed in the data. The
             analysis results are interpreted in terms of
             model-independent limits and used to derive exclusion limits
             on the masses of the top squark t1 and the tau slepton τ1
             in a simplified model of supersymmetry with a nearly
             massless gravitino. In this model, masses up to m(t1)=1.16
             TeV and m(τ1)=1.00 TeV are excluded at 95% confidence
             level.},
   Doi = {10.1103/PhysRevD.98.032008},
   Key = {fds356673}
}

@article{fds353613,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
             KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA},
   Title = {Search for top squarks in events with a Higgs or Z boson
             using 139 fb - 1 of pp collision data at √s=13
             TeV with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {11},
   Year = {2020},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-08469-8},
   Abstract = {This paper presents a search for direct top squark pair
             production in events with missing transverse momentum plus
             either a pair of jets consistent with Standard Model Higgs
             boson decay into b-quarks or a same-flavour opposite-sign
             dilepton pair with an invariant mass consistent with a Z
             boson. The analysis is performed using the proton–proton
             collision data at s=13 TeV collected with the ATLAS detector
             during the LHC Run-2, corresponding to an integrated
             luminosity of 139 fb- 1. No excess is observed in the data
             above the Standard Model predictions. The results are
             interpreted in simplified models featuring direct production
             of pairs of either the lighter top squark (t~ 1) or the
             heavier top squark (t~ 2), excluding at 95% confidence level
             t~ 1 and t~ 2 masses up to about 1220 and 875 GeV,
             respectively.},
   Doi = {10.1140/epjc/s10052-020-08469-8},
   Key = {fds353613}
}

@article{fds321099,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Search for top squarks in final states with one isolated
             lepton, jets, and missing transverse momentum in s =13 TeV
             pp collisions with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.052009},
   Abstract = {The results of a search for the top squark, the
             supersymmetric partner of the top quark, in final states
             with one isolated electron or muon, jets, and missing
             transverse momentum are reported. The search uses the 2015
             LHC pp collision data at a center-of-mass energy of s=13 TeV
             recorded by the ATLAS detector and corresponding to an
             integrated luminosity of 3.2 fb-1. The analysis targets two
             types of signal models: gluino-mediated pair production of
             top squarks with a nearly mass-degenerate top squark and
             neutralino and direct pair production of top squarks,
             decaying to the top quark and the lightest neutralino. The
             experimental signature in both signal scenarios is similar
             to that of a top quark pair produced in association with
             large missing transverse momentum. No significant excess
             over the Standard Model background prediction is observed,
             and exclusion limits on gluino and top squark masses are set
             at 95% confidence level. The results extend the LHC run-1
             exclusion limit on the gluino mass up to 1460 GeV in the
             gluino-mediated scenario in the high gluino and low top
             squark mass region and add an excluded top squark mass
             region from 745 to 780 GeV for the direct top squark model
             with a massless lightest neutralino. The results are also
             reinterpreted to set exclusion limits in a model of
             vectorlike top quarks.},
   Doi = {10.1103/PhysRevD.94.052009},
   Key = {fds321099}
}

@article{fds356597,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA},
   Title = {Search for top-quark decays t → Hq with 36
             fb−1 of pp collision data at √s = 13 TeV with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {5},
   Year = {2019},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2019)123},
   Abstract = {A search for flavour-changing neutral current decays of a
             top quark into an up-type quark (q = u, c) and the Standard
             Model Higgs boson, t → Hq, is presented. The search is
             based on a dataset of pp collisions at s = 13 TeV recorded
             in 2015 and 2016 with the ATLAS detector at the CERN Large
             Hadron Collider and corresponding to an integrated
             luminosity of 36.1 fb−1. Two complementary analyses are
             performed to search for top-quark pair events in which one
             top quark decays into Wb and the other top quark decays into
             Hq, and target the H→ bb¯ and H → τ+τ− decay modes,
             respectively. The high multiplicity of b-quark jets, or the
             presence of hadronically decaying τ-leptons, is exploited
             in the two analyses respectively. Multivariate techniques
             are used to separate the signal from the background, which
             is dominated by top-quark pair production. No significant
             excess of events above the background expectation is found,
             and 95% CL upper limits on the t → Hq branching ratios are
             derived. The combination of these searches with ATLAS
             searches in diphoton and multilepton final states yields
             observed (expected) 95% CL upper limits on the t → Hc and
             t → Hu branching ratios of 1.1 × 10−3 (8.3 × 10−4)
             and 1.2 × 10−3 (8.3 × 10−4), respectively. The
             corresponding combined observed (expected) upper limits on
             the |λtcH| and |λtuH| couplings are 0.064 (0.055) and
             0.066 (0.055), respectively.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP05(2019)123},
   Key = {fds356597}
}

@article{fds307955,
   Author = {Aaltonen, T and others},
   Title = {Search for Top-Quark Production via Flavor-Changing Neutral
             Currents in W + 1 Jet Events at CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {15},
   Pages = {151801},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.151801},
   Abstract = {We report on a search for the non-standard-model process
             u(c) + g --> t using pp[over ] collision data collected by
             the Collider Detector at Fermilab II detector corresponding
             to 2.2 fb;{-1}. The candidate events are classified as
             signal-like or backgroundlike by an artificial neural
             network. The observed discriminant distribution yields no
             evidence for flavor-changing neutral current top-quark
             production, resulting in an upper limit on the production
             cross section sigma(u(c) + g --> t) < 1.8 pb at the 95% C.L.
             Using theoretical predictions we convert the cross section
             limit to upper limits on flavor-changing neutral current
             branching ratios: B(t --> u + g) < 3.9 x 10;{-4} and B(t -->
             c + g) < 5.7 x 10;{-3}.},
   Doi = {10.1103/physrevlett.102.151801},
   Key = {fds307955}
}

@article{fds336452,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for top-squark pair production in final states with
             one lepton, jets, and missing transverse momentum using 36
             fb−1 of √s=13 TeV pp collision data with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2018},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2018)108},
   Abstract = {The results of a search for the direct pair production of
             top squarks, the supersymmetric partner of the top quark, in
             final states with one isolated electron or muon, several
             energetic jets, and missing transverse momentum are
             reported. The analysis also targets spin-0 mediator models,
             where the mediator decays into a pair of dark-matter
             particles and is produced in association with a pair of top
             quarks. The search uses data from proton-proton collisions
             delivered by the Large Hadron Collider in 2015 and 2016 at a
             centre-of-mass energy of s=13 TeV and recorded by the ATLAS
             detector, corresponding to an integrated luminosity of 36
             fb−1. A wide range of signal scenarios with different
             mass-splittings between the top squark, the lightest
             neutralino and possible intermediate supersymmetric
             particles are considered, including cases where the W bosons
             or the top quarks produced in the decay chain are off-shell.
             No significant excess over the Standard Model prediction is
             observed. The null results are used to set exclusion limits
             at 95% confidence level in several supersymmetry benchmark
             models. For pair-produced top-squarks decaying into top
             quarks, top-squark masses up to 940 GeV are excluded.
             Stringent exclusion limits are also derived for all other
             considered top-squark decay scenarios. For the spin-0
             mediator models, upper limits are set on the visible
             cross-section.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP06(2018)108},
   Key = {fds336452}
}

@article{fds347494,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
             De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
             MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister,
             I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba,
             LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret,
             M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo,
             F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
             Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M},
   Title = {Search for triboson [Formula: see text] production in
             pp collisions at [Formula: see text] [Formula: see
             text] with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {3},
   Pages = {141},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-4692-1},
   Abstract = {This paper reports a search for triboson [Formula: see text]
             production in two decay channels ([Formula: see text] and
             [Formula: see text] with [Formula: see text]) in
             proton-proton collision data corresponding to an integrated
             luminosity of 20.3 [Formula: see text] at a centre-of-mass
             energy of 8 [Formula: see text] with the ATLAS detector at
             the Large Hadron Collider. Events with exactly three charged
             leptons, or two leptons with the same electric charge in
             association with two jets, are selected. The total number of
             events observed in data is consistent with the Standard
             Model (SM) predictions. The observed 95% confidence level
             upper limit on the SM [Formula: see text] production cross
             section is found to be 730 fb with an expected limit of 560
             fb in the absence of SM [Formula: see text] production.
             Limits are also set on <i>WWWW</i> anomalous quartic gauge
             couplings.},
   Doi = {10.1140/epjc/s10052-017-4692-1},
   Key = {fds347494}
}

@booklet{Abbott98n,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
             EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis,
             E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram,
             I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
             W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
             G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
   Title = {Search for trilepton signatures from associated gaugino pair
             production},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {8},
   Pages = {1591-1596},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.1591},
   Abstract = {We report on a search for the trilepton decay signature from
             the associated production of supersymmetric gaugino pairs,
             χ∼±1χ∼02, within the context of minimal
             supersymmetric models that conserve R parity. This search
             uses 95 pb−1 of pp− data taken at s = 1.8 TeV with the
             D0 detector. No evidence of a trilepton signature has been
             found, and a limit on the product of cross section times
             branching fraction to trileptons is given as a function of
             χ∼±1 mass. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.80.1591},
   Key = {Abbott98n}
}

@article{fds221244,
   Author = {A.V. Kotwal and G. Aad et al (ATLAS Collaboration)},
   Title = {Search for ttbar resonances in the lepton plus jets final
             state with ATLAS using 4.7 / fb of pp collisions at
             sqrt(s)=7  TeV},
   Journal = {Phys. Rev. D},
   Volume = {88},
   Number = {012004},
   Year = {2013},
   Month = {July},
   Key = {fds221244}
}

@article{fds352786,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
             Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C},
   Title = {Search for tt¯ resonances in fully hadronic final states in
             pp collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2020},
   Number = {10},
   Year = {2020},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2020)061},
   Abstract = {This paper presents a search for new heavy particles
             decaying into a pair of top quarks using 139 fb−1 of
             proton-proton collision data recorded at a centre-of-mass
             energy of s = 13 TeV with the ATLAS detector at the Large
             Hadron Collider. The search is performed using events
             consistent with pair production of high-transverse-momentum
             top quarks and their subsequent decays into the fully
             hadronic final states. The analysis is optimized for
             resonances decaying into a tt¯ pair with mass above 1.4
             TeV, exploiting a dedicated multivariate technique with jet
             substructure to identify hadronically decaying top quarks
             using large-radius jets and evaluating the background
             expectation from data. No significant deviation from the
             background prediction is observed. Limits are set on the
             production cross-section times branching fraction for the
             new Z′ boson in a topcolor-assisted-technicolor model. The
             Z′ boson masses below 3.9 and 4.7 TeV are excluded at 95%
             confidence level for the decay widths of 1% and 3%,
             respectively. [Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP10(2020)061},
   Key = {fds352786}
}

@article{fds307590,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Search for tt̄ resonances in the lepton plus jets final
             state with ATLAS using 4.7 fb–1of pp collisions
             at √s = 7 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.012004},
   Abstract = {A search for new particles that decay into top quark pairs
             (tt) is performed with the ATLAS experiment at the LHC using
             an integrated luminosity of 4.7 fb–1of proton–proton
             (pp) collision data collected at a center-of-mass energy
             √s = 7 TeV. In the tt̄→ WbWb decay, the lepton plus
             jets final state is used, where one W boson decays
             leptonically and the other hadronically. The tt̄system is
             reconstructed using both small-radius and large-radius jets,
             the latter being supplemented by a jet substructure
             analysis. A search for local excesses in the number of data
             events compared to the Standard Model expectation in the
             tt̄invariant mass spectrum is performed. No evidence for a
             tt̄resonance is found and 95% credibility-level limits on
             the production rate are determined for massive states
             predicted in two benchmark models. The upper limits on the
             cross section times branching ratio of a narrow Z′
             resonance range from 5.1 pb for a boson mass of 0.5 TeV to
             0.03 pb for a mass of 3 TeV. A narrow leptophobic topcolor
             Z′ resonance with a mass below 1.74 TeV is excluded.
             Limits are also derived for a broad color-octet resonance
             with Γ/m = 15.3%. A Kaluza–Klein excitation of the gluon
             in a Randall–Sundrum model is excluded for masses below
             2.07 TeV.},
   Doi = {10.1103/PhysRevD.88.012004},
   Key = {fds307590}
}

@article{fds355554,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
             KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
   Title = {Search for type-III seesaw heavy leptons in dilepton final
             states in pp collisions at √s=13TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {81},
   Number = {3},
   Year = {2021},
   Month = {March},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-08929-9},
   Abstract = {A search for the pair production of heavy leptons as
             predicted by the type-III seesaw mechanism is presented. The
             search uses proton–proton collision data at a
             centre-of-mass energy of 13 TeV, corresponding to 139fb-1
             of integrated luminosity recorded by the ATLAS detector
             during Run 2 of the Large Hadron Collider. The analysis
             focuses on the final state with two light leptons (electrons
             or muons) of different flavour and charge combinations, with
             at least two jets and large missing transverse momentum. No
             significant excess over the Standard Model expectation is
             observed. The results are translated into exclusion limits
             on heavy-lepton masses, and the observed lower limit on the
             mass of the type-III seesaw heavy leptons is 790 GeV at 95%
             confidence level.},
   Doi = {10.1140/epjc/s10052-021-08929-9},
   Key = {fds355554}
}

@article{fds367719,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
             SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
             Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Alconada
             Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
             M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
             JF},
   Title = {Search for type-III seesaw heavy leptons in leptonic final
             states in pp collisions at √s=13TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {82},
   Number = {11},
   Year = {2022},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-022-10785-0},
   Abstract = {A search for the pair production of heavy leptons as
             predicted by the type-III seesaw mechanism is presented. The
             search uses proton–proton collision data at a
             centre-of-mass energy of 13 TeV, corresponding to 139fb-1
             of integrated luminosity recorded by the ATLAS detector
             during Run 2 of the Large Hadron Collider. The analysis
             focuses on final states with three or four electrons or
             muons from the possible decays of new heavy leptons via
             intermediate electroweak bosons. No significant deviations
             above the Standard Model expectation are observed; upper and
             lower limits on the heavy lepton production cross-section
             and masses are derived respectively. These results are then
             combined for the first time with the ones already published
             by ATLAS using the channel with two leptons in the final
             state. The observed lower limit on the mass of the type-III
             seesaw heavy leptons combining two, three and four lepton
             channels together is 910 GeV at the 95% confidence
             level.},
   Doi = {10.1140/epjc/s10052-022-10785-0},
   Key = {fds367719}
}

@article{fds310267,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for type-III seesaw heavy leptons in pp collisions at
             s =8 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.032001},
   Abstract = {A search for the pair production of heavy leptons (N0,L±)
             predicted by the type-III seesaw theory formulated to
             explain the origin of small neutrino masses is presented.
             The decay channels N0→W±l (=e,μ,τ) and L±→W±ν
             (ν=νe,νμ,ντ) are considered. The analysis is performed
             using the final state that contains two leptons (electrons
             or muons), two jets from a hadronically decaying W boson and
             large missing transverse momentum. The data used in the
             measurement correspond to an integrated luminosity of 20.3
             fb-1 of pp collisions at s=8 TeV collected by the ATLAS
             detector at the LHC. No evidence of heavy lepton pair
             production is observed. Heavy leptons with masses below
             325-540 GeV are excluded at the 95% confidence level,
             depending on the theoretical scenario considered.},
   Doi = {10.1103/PhysRevD.92.032001},
   Key = {fds310267}
}

@article{fds308062,
   Author = {Abulencia, and A, and others},
   Title = {Search for V + A current in top quark decay in p anti-p
             collisions at s**(1/2) = 1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {7},
   Pages = {072001},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.072001},
   Abstract = {We report an upper limit on the fraction of V+A current,
             fV+A, in top-quark decays, using approximately 700 pb-1 of
             p[overline p] collisions at sqrt(s)=1.96 TeV acquired by the
             upgraded Collider Detector at Fermilab. For the decay
             t-->Wb-->[script-l]nub (where [script-l]=e or µ), the
             invariant mass of the charged lepton and the bottom quark
             jet is sensitive to the polarization of the W boson. We
             determine fV+A=-0.06$\pm$0.25 given a top-quark mass of 175
             GeV/c2. We set an upper limit on fV+A of 0.29 at the 95\%
             confidence level, an improvement by a factor of 2 on the
             previous best direct limit.},
   Doi = {10.1103/physrevlett.98.072001},
   Key = {fds308062}
}

@article{fds356630,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
             C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
             RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
   Title = {Search for vector-boson resonances decaying to a top quark
             and bottom quark in the lepton plus jets final state in pp
             collisions at √s=13TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {788},
   Pages = {347-370},
   Year = {2019},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.11.032},
   Abstract = {A search for new charged massive gauge bosons, W′, is
             performed with the ATLAS detector at the LHC. Data were
             collected in proton–proton collisions at a center-of-mass
             energy of s=13 TeV and correspond to an integrated
             luminosity of 36.1 fb−1. This analysis searches for W′
             bosons in the W′→tb¯ decay channel in final states with
             an electron or muon plus jets. The search covers resonance
             masses between 0.5 and 5.0 TeV and considers right-handed
             W′ bosons. No significant deviation from the Standard
             Model (SM) expectation is observed and upper limits are set
             on the W′→tb¯ cross section times branching ratio and
             the W′ boson effective couplings as a function of the W′
             boson mass. For right-handed W′ bosons with coupling to
             the SM particles equal to the SM weak coupling constant,
             masses below 3.15 TeV are excluded at the 95% confidence
             level. This search is also combined with a previously
             published ATLAS result for W′→tb¯ in the fully hadronic
             final state. Using the combined searches, right-handed W′
             bosons with masses below 3.25 TeV are excluded at the 95%
             confidence level.},
   Doi = {10.1016/j.physletb.2018.11.032},
   Key = {fds356630}
}

@article{fds310281,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G},
   Title = {Search for vectorlike B quarks in events with one isolated
             lepton, missing transverse momentum, and jets at s =8 TeV
             with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.112011},
   Abstract = {A search has been performed for pair production of heavy
             vectorlike down-type (B) quarks. The analysis explores the
             lepton-plus-jets final state, characterized by events with
             one isolated charged lepton (electron or muon), significant
             missing transverse momentum, and multiple jets. One or more
             jets are required to be tagged as arising from b quarks, and
             at least one pair of jets must be tagged as arising from the
             hadronic decay of an electroweak boson. The analysis uses
             the full data sample of pp collisions recorded in 2012 by
             the ATLAS detector at the LHC, operating at a center-of-mass
             energy of 8 TeV, corresponding to an integrated luminosity
             of 20.3 fb-1. No significant excess of events is observed
             above the expected background. Limits are set on vectorlike
             B production, as a function of the B branching ratios,
             assuming the allowable decay modes are B→Wt/Zb/Hb. In the
             chiral limit with a branching ratio of 100% for the decay
             B→Wt, the observed (expected) 95% C.L. lower limit on the
             vectorlike B mass is 810 GeV (760 GeV). In the case where
             the vectorlike B quark has branching ratio values
             corresponding to those of an SU(2) singlet state, the
             observed (expected) 95% C.L. lower limit on the vectorlike B
             mass is 640 GeV (505 GeV). The same analysis, when used to
             investigate pair production of a colored, charge 5/3 exotic
             fermion T5/3, with subsequent decay T5/3→Wt, sets an
             observed (expected) 95% C.L. lower limit on the T5/3 mass of
             840 GeV (780 GeV).},
   Doi = {10.1103/PhysRevD.91.112011},
   Key = {fds310281}
}

@article{fds356691,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for W W/W Z resonance production in ℓνqq final
             states in pp collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {3},
   Year = {2018},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2018)042},
   Abstract = {A search is conducted for new resonances decaying into a W W
             or W Z boson pair, where one W boson decays leptonically and
             the other W or Z boson decays hadronically. It is based on
             proton-proton collision data with an integrated luminosity
             of 36.1 fb−1 collected with the ATLAS detector at the
             Large Hadron Collider at a centre-of-mass energy of s=13 TeV
             in 2015 and 2016. The search is sensitive to diboson
             resonance production via vector-boson fusion as well as
             quark-antiquark annihilation and gluon-gluon fusion
             mechanisms. No significant excess of events is observed with
             respect to the Standard Model backgrounds. Several benchmark
             models are used to interpret the results. Limits on the
             production cross section are set for a new narrow scalar
             resonance, a new heavy vector-boson and a spin-2
             Kaluza-Klein graviton.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP03(2018)042},
   Key = {fds356691}
}

@article{fds310313,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V},
   Title = {Search for W ′ → t b ¯ in the lepton plus jets final
             state in proton–proton collisions at a centre-of-mass
             energy of s = 8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {743},
   Pages = {235-255},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.02.051},
   Abstract = {A search for new charged massive gauge bosons, called W′,
             is performed with the ATLAS detector at the LHC, in
             proton–proton collisions at a centre-of-mass energy of s=8
             TeV, using a dataset corresponding to an integrated
             luminosity of 20.3 fb−1. This analysis searches for W′
             bosons in the W′→tb¯ decay channel in final states with
             electrons or muons, using a multivariate method based on
             boosted decision trees. The search covers masses between 0.5
             and 3.0 TeV, for right-handed or left-handed W′ bosons. No
             significant deviation from the Standard Model expectation is
             observed and limits are set on the W′→tb¯ cross-section
             times branching ratio and on the W′-boson effective
             couplings as a function of the W′-boson mass using the CLs
             procedure. For a left-handed (right-handed) W′ boson,
             masses below 1.70 (1.92) TeV are excluded at 95% confidence
             level.},
   Doi = {10.1016/j.physletb.2015.02.051},
   Key = {fds310313}
}

@article{fds308078,
   Author = {Abulencia, and A, and others},
   Title = {Search for W' boson decaying to electron-neutrino pairs in p
             anti-p collisions at s**(1/2) = 1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {9},
   Pages = {091101},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.091101},
   Abstract = {We present the results of a search for W[prime] boson
             decaying to electron-neutrino pairs in p[overline p]
             collisions at a center-of-mass energy of 1.96 TeV, using a
             data sample corresponding to 205 pb-1 of integrated
             luminosity collected by the CDF II detector at Fermilab. We
             observe no evidence for this decay mode and set limits on
             the production cross section times branching fraction,
             assuming the neutrinos from W[prime] boson decays to be
             light. If we assume the manifest left-right symmetric model,
             we exclude a W[prime] boson with mass less than 788 GeV/c2
             at the 95\% confidence level.},
   Doi = {10.1103/PhysRevD.75.091101},
   Key = {fds308078}
}

@article{fds307605,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
   Title = {Search for WH production with a light Higgs boson decaying
             to prompt electron-jets in proton-proton collisions at
             √s=7 TeV with the ATLAS detector},
   Journal = {New Journal of Physics},
   Volume = {15},
   Number = {4},
   Pages = {043009-043009},
   Publisher = {IOP Publishing},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1088/1367-2630/15/4/043009},
   Abstract = {A search is performed for WH production with a light Higgs
             boson decaying to hidden-sector particles resulting in
             clusters of collimated electrons, known as electron-jets.
             The search is performed with 2.04 fb-1 of data collected in
             2011 with the ATLAS detector at the Large Hadron Collider in
             proton-proton collisions at . One event satisfying the
             signal selection criteria is observed, which is consistent
             with the expected background rate. Limits on the product of
             the WH production cross section and the branching ratio of a
             Higgs boson decaying to prompt electron-jets are calculated
             as a function of a Higgs boson mass in the range from 100 to
             140 GeV. © CERN 2013 for the benefit of the ATLAS
             Collaboration, published under the terms of the Creative
             Commons Attribution 3.0 licence by IOP Publishing Ltd and
             Deutsche Physikalische Gesellschaft. Any further
             distribution of this work must maintain attribution to the
             author(s) and the published article's title, journal
             citation and DOI.},
   Doi = {10.1088/1367-2630/15/4/043009},
   Key = {fds307605}
}

@article{fds307995,
   Author = {Aaltonen, T and others},
   Title = {Search for WW and WZ production in lepton plus jets final
             state at CDF},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {11},
   Pages = {112011},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.112011},
   Abstract = {We present a search for WW and WZ production in final states
             that contain a charged lepton (electron or muon) and at
             least two jets, produced in sqrt[s]=1.96  TeV pp̅
             collisions at the Fermilab Tevatron, using data
             corresponding to 1.2  fb-1 of integrated luminosity
             collected with the CDF II detector. Diboson production in
             this decay channel has yet to be observed at hadron
             colliders due to the large single W plus jets background. An
             artificial neural network has been developed to increase
             signal sensitivity, as compared with an event selection
             based on conventional cuts. We set a 95% confidence level
             upper limit of σWW×BR(W→ℓνℓ,W→jets)+σWZ×BR(W→ℓνℓ,Z→jets)&lt;2.88  pb,
             which is consistent with the standard model
             next-to-leading-order cross section calculation for this
             decay channel of 2.09 &plusmn; 0.12  pb.},
   Doi = {10.1103/PhysRevD.79.112011},
   Key = {fds307995}
}

@article{fds310351,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for WZ resonances in the fully leptonic channel using
             pp collisions at s=8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {737},
   Pages = {223-243},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.08.039},
   Abstract = {A search for resonant WZ production in the ℓνℓ'ℓ'
             (ℓ,ℓ'=e,μ) decay channel using 20.3 fb-1 of s=8TeV pp
             collision data collected by the ATLAS experiment at LHC is
             presented. No significant deviation from the Standard Model
             prediction is observed and upper limits on the production
             cross sections of WZ resonances from an extended gauge model
             W' and from a simplified model of heavy vector triplets are
             derived. A corresponding observed (expected) lower mass
             limit of 1.52 (1.49) TeV is derived for the W' at the 95%
             confidence level. © 2014 Elsevier B.V.},
   Doi = {10.1016/j.physletb.2014.08.039},
   Key = {fds310351}
}

@article{fds307806,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca almenar, C and Cuevas, J and Culbertson, R and Dagenhart, D},
   Title = {Search for WZ+ZZ production with missing transverse
             energy+jets with b enhancement at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012002},
   Abstract = {Diboson production (WW+WZ+ZZ) has been observed at the
             Tevatron in hadronic decay modes dominated by the WW
             process. This paper describes the measurement of the cross
             section of WZ and ZZ events in final states with large E T
             and using b-jet identification as a tool to suppress WW
             contributions. Because of the limited energy resolution, we
             cannot distinguish between partially hadronic decays of WZ
             and ZZ, and we measure the sum of these processes. The
             number of signal events is extracted using a simultaneous
             fit to the invariant mass distribution of the two jets for
             events with two b-jet candidates and events with fewer than
             two b-jet candidates. We measure a cross section
             σ(pp̄→WZ,ZZ)=5.8-3.0+3.6pb, in agreement with the
             standard model. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.85.012002},
   Key = {fds307806}
}

@article{fds356679,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik,
             Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli,
             E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
             Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
             V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Search for W′  →  tb decays in the hadronic final
             state using pp collisions at √s=13TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {781},
   Pages = {327-348},
   Year = {2018},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.03.036},
   Abstract = {A search for W′-boson production in the
             W′→tb¯→qq¯′bb¯ decay channel is presented using
             36.1fb−1 of 13 TeV proton–proton collision data
             collected by the ATLAS detector at the Large Hadron Collider
             in 2015 and 2016. The search is interpreted in terms of both
             a left-handed and a right-handed chiral W′ boson within
             the mass range 1–5 TeV. Identification of the hadronically
             decaying top quark is performed using jet substructure
             tagging techniques based on a shower deconstruction
             algorithm. No significant deviation from the Standard Model
             prediction is observed and the results are expressed as
             upper limits on the W′→tb¯ production cross-section
             times branching ratio as a function of the W′-boson mass.
             These limits exclude W′ bosons with right-handed couplings
             with masses below 3.0 TeV and W′ bosons with left-handed
             couplings with masses below 2.9 TeV, at the 95% confidence
             level.},
   Doi = {10.1016/j.physletb.2018.03.036},
   Key = {fds356679}
}

@article{fds308140,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
             AG and Clark, D and Coca, M and Connolly, A},
   Title = {Search for ZZ and ZW production in pp̄ collisions at
             s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {9},
   Pages = {1-7},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.091105},
   Abstract = {We present a search for ZZ and ZW vector boson pair
             production in pp̄ collisions at s=1.96TeV using the
             leptonic decay channels ZZ→llνν, ZZ→lll′l′, and
             ZW→lll′ν. In a data sample corresponding to an
             integrated luminosity of 194pb-1 collected with the Collider
             Detector at Fermilab, 3 candidate events are found with an
             expected background of 1.0±0.2 events. We set a 95%
             confidence level upper limit of 15.2pb on the cross section
             for ZZ plus ZW production, compared to the standard model
             prediction of 5.0±0.4pb. © 2005 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.71.091105},
   Key = {fds308140}
}

@article{fds310321,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Search for [Formula: see text] decays in [Formula: see text]
             collisions at [Formula: see text] = 8 TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {4},
   Pages = {165},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3372-2},
   Abstract = {A search for a massive [Formula: see text] gauge boson
             decaying to a top quark and a bottom quark is performed with
             the ATLAS detector in [Formula: see text] collisions at the
             LHC. The dataset was taken at a centre-of-mass energy of
             [Formula: see text] and corresponds to [Formula: see text]
             of integrated luminosity. This analysis is done in the
             hadronic decay mode of the top quark, where novel jet
             substructure techniques are used to identify jets from
             high-momentum top quarks. This allows for a search for
             high-mass [Formula: see text] bosons in the range
             1.5-3.0 [Formula: see text]. [Formula: see text]-tagging is
             used to identify jets originating from [Formula: see
             text]-quarks. The data are consistent with Standard Model
             background-only expectations, and upper limits at 95 %
             confidence level are set on the [Formula: see text] cross
             section times branching ratio ranging from [Formula: see
             text] to [Formula: see text] for left-handed [Formula: see
             text] bosons, and ranging from [Formula: see text] to
             [Formula: see text] for [Formula: see text] bosons with
             purely right-handed couplings. Upper limits at 95 %
             confidence level are set on the [Formula: see text]-boson
             coupling to [Formula: see text] as a function of the
             [Formula: see text] mass using an effective field theory
             approach, which is independent of details of particular
             models predicting a [Formula: see text] boson.},
   Doi = {10.1140/epjc/s10052-015-3372-2},
   Key = {fds310321}
}

@article{fds307880,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for {Randall-Sundrum} gravitons in the diphoton
             channel at {CDF}},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {1},
   Pages = {011102},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.011102},
   Abstract = {We report on a search for new particles in the diphoton
             channel using a data sample of pp̄ collisions at
             √s=1.96TeV collected by the CDF II detector at the
             Fermilab Tevatron, with an integrated luminosity of
             5.4fb⊃-1. The diphoton invariant mass spectrum of the data
             agrees well with the standard model expectation. We set
             upper limits on the production cross section times branching
             ratio for the Randall-Sundrum graviton, as a function of
             diphoton mass. We subsequently derive lower limits on the
             graviton mass of 459GeV/c2 and 963GeV/c2, at the 95%
             confidence level, for coupling parameters (k/M̄Pl) of 0.01
             and 0.1, respectively. © 2011 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.83.011102},
   Key = {fds307880}
}

@article{fds373467,
   Author = {Amerl, M and Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk
             Cakir, I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin,
             T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi,
             G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori,
             G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang,
             R and Zhang, J and Berlendis, S and Cheu, E and Cui, Z and Ghosh, A and Johns,
             KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand,
             HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK},
   Title = {Search in diphoton and dielectron final states for displaced
             production of Higgs or Z bosons with the ATLAS detector in
             Formula Presented pp collisions},
   Journal = {Physical Review D},
   Volume = {108},
   Number = {1},
   Year = {2023},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.108.012012},
   Abstract = {A search is presented for displaced production of Higgs
             bosons or Z bosons, originating from the decay of a neutral
             long-lived particle (LLP) and reconstructed in the decay
             modes H → γ γ and Z → e e . The analysis uses the full
             Run 2 dataset of proton-proton collisions delivered by the
             LHC at an energy of s = 13 TeV between 2015 and 2018 and
             recorded by the ATLAS detector, corresponding to an
             integrated luminosity of 139 fb - 1 . Exploiting the
             capabilities of the ATLAS liquid argon calorimeter to
             precisely measure the arrival times and trajectories of
             electromagnetic objects, the analysis searches for the
             signature of pairs of photons or electrons which arise from
             a common displaced vertex and which arrive after some delay
             at the calorimeter. The results are interpreted in a
             gauge-mediated supersymmetry breaking model with
             pair-produced Higgsinos that decay to LLPs, and each LLP
             subsequently decays into either a Higgs boson or a Z boson.
             The final state includes at least two particles that escape
             direct detection, giving rise to missing transverse
             momentum. No significant excess is observed above the
             background expectation. The results are used to set upper
             limits on the cross section for Higgsino pair production, up
             to a χ ˜ 1 0 mass of 369 (704) GeV for decays with 100%
             branching ratio of χ ˜ 1 0 to Higgs ( Z ) bosons for a χ
             ˜ 1 0 lifetime of 2 ns. A model-independent limit is also
             set on the production of pairs of photons or electrons with
             a significant delay in arrival at the calorimeter.},
   Doi = {10.1103/PhysRevD.108.012012},
   Key = {fds373467}
}

@article{fds308065,
   Author = {Aaltonen, T and others},
   Title = {Searches for direct pair production of supersymmetric top
             and supersymmetric bottom quarks in p[overline p] collisions
             at $\sqrt{s}$=1.96 TeV},
   Journal = {Phys. Rev.},
   Volume = {D76},
   Number = {7},
   Pages = {072010},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.76.072010},
   Abstract = {We search for direct pair production of supersymmetric top
             quarks and supersymmetric bottom quarks in proton-antiproton
             collisions at sqrt(s)=1.96 TeV, using 295 pb-1 of data
             recorded by the Collider Detector at Fermilab (CDF II)
             experiment. The supersymmetric top (supersymmetric bottom)
             quarks are selected by reconstructing their decay into a
             charm (bottom) quark and a neutralino, which is assumed to
             be the lightest supersymmetric particle. The signature of
             such processes is two energetic heavy-flavor jets and
             missing transverse energy. The number of events that pass
             our selection for each search process is consistent with the
             expected standard model background. By comparing our results
             to the theoretical production cross sections of the
             supersymmetric top and supersymmetric bottom quarks in the
             minimal supersymmetric standard model, we exclude, at a 95%
             confidence level in the frame of that model, a
             supersymmetric top quark mass up to 132 GeV/c2 for a
             neutralino mass of 48 GeV/c2, and a supersymmetric bottom
             quark mass up to 193 GeV/c2 for a neutralino mass of 40
             GeV/c2.},
   Doi = {10.1103/PhysRevD.76.072010},
   Key = {fds308065}
}

@article{fds349429,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA},
   Title = {Searches for electroweak production of supersymmetric
             particles with compressed mass spectra in s =13 TeV pp
             collisions with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {101},
   Number = {5},
   Year = {2020},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.101.052005},
   Abstract = {This paper presents results of searches for the electroweak
             production of supersymmetric particles in models with
             compressed mass spectra. The searches use 139 fb-1 of s=13
             TeV proton-proton collision data collected by the ATLAS
             experiment at the Large Hadron Collider. Events with missing
             transverse momentum and two same-flavor, oppositely charged,
             low-transverse-momentum leptons are selected, and are
             further categorized by the presence of hadronic activity
             from initial-state radiation or a topology compatible with
             vector-boson fusion processes. The data are found to be
             consistent with predictions from the Standard Model. The
             results are interpreted using simplified models of
             R-parity-conserving supersymmetry in which the lightest
             supersymmetric partner is a neutralino with a mass similar
             to the lightest chargino, the second-to-lightest neutralino,
             or the slepton. Lower limits on the masses of charginos in
             different simplified models range from 193 to 240 GeV for
             moderate mass splittings, and extend down to mass splittings
             of 1.5 to 2.4 GeV at the LEP chargino bounds (92.4 GeV).
             Similar lower limits on degenerate light-flavor sleptons
             extend up to masses of 251 GeV and down to mass splittings
             of 550 MeV. Constraints on vector-boson fusion production of
             electroweak SUSY states are also presented.},
   Doi = {10.1103/PhysRevD.101.052005},
   Key = {fds349429}
}

@article{fds372743,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
             A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
             MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames,
             CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche,
             CS and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena,
             E},
   Title = {Searches for exclusive Higgs and Z boson decays into a
             vector quarkonium state and a photon using 139 fb -
             1 of ATLAS √s=13 TeV proton–proton collision
             data},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {9},
   Year = {2023},
   Month = {September},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11869-1},
   Abstract = {Searches for the exclusive decays of Higgs and Z bosons into
             a vector quarkonium state and a photon are performed in the
             μ+μ-γ final state with a proton–proton collision data
             sample corresponding to an integrated luminosity of 139 fb
             - 1 collected at s=13 TeV with the ATLAS detector at the
             CERN Large Hadron Collider. The observed data are compatible
             with the expected backgrounds. The 95% confidence-level
             upper limits on the branching fractions of the Higgs boson
             decays into J/ψγ , ψ(2S)γ , and Υ(1S,2S,3S)γ are found
             to be 2.0 × 10 - 4 , 10.5 × 10 - 4 , and (2.5 , 4.2 , 3.4)
             × 10 - 4 , respectively, assuming Standard Model production
             of the Higgs boson. The corresponding 95% CL upper limits on
             the branching fractions of the Z boson decays are 1.2 × 10
             - 6 , 2.4 × 10 - 6 , and (1.1 , 1.3 , 2.4) × 10 - 6 . An
             observed 95% CL interval of (- 133 , 175) is obtained for
             the κc/ κγ ratio of Higgs boson coupling modifiers, and a
             95% CL interval of (- 37 , 40) is obtained for κb/ κγ
             .},
   Doi = {10.1140/epjc/s10052-023-11869-1},
   Key = {fds372743}
}

@article{fds356639,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Searches for exclusive Higgs and Z boson decays into
             J/ψ γ, ψ(2S) γ, and ϒ(nS) γ at s=13TeV with the
             ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {786},
   Pages = {134-155},
   Year = {2018},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2018.09.024},
   Abstract = {Searches for the exclusive decays of the Higgs and Z bosons
             into a J/ψ, ψ(2S), or ϒ(nS) (n=1,2,3) meson and a photon
             are performed with a pp collision data sample corresponding
             to an integrated luminosity of 36.1fb−1 collected at
             s=13TeV with the ATLAS detector at the CERN Large Hadron
             Collider. No significant excess of events is observed above
             the expected backgrounds, and 95% confidence-level upper
             limits on the branching fractions of the Higgs boson decays
             to J/ψγ, ψ(2S)γ, and ϒ(nS)γ of 3.5×10−4,
             2.0×10−3, and (4.9,5.9,5.7)×10−4, respectively, are
             obtained assuming Standard Model production. The
             corresponding 95% confidence-level upper limits for the
             branching fractions of the Z boson decays are 2.3×10−6,
             4.5×10−6 and (2.8,1.7,4.8)×10−6, respectively.},
   Doi = {10.1016/j.physletb.2018.09.024},
   Key = {fds356639}
}

@article{fds321097,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Searches for heavy diboson resonances in pp collisions at
             √s=13 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2016)173},
   Abstract = {Searches for new heavy resonances decaying to WW, WZ, and ZZ
             bosons are presented, using a data sample corresponding to
             3.2 fb−1 of pp collisions at s=13 TeV collected with the
             ATLAS detector at the CERN Large Hadron Collider. Analyses
             selecting ννqq, ℓνqq, ℓℓqq and qqqq final states
             are combined, searching for an arrow-width resonance with
             mass between 500 and 3000 GeV. The discriminating variable
             is either an invariant mass or a transverse mass. No
             significant deviations from the Standard Model predictions
             are observed. Three benchmark models are tested: a model
             predicting the existence of a new heavy scalar singlet, a
             simplified model predicting a heavy vector-boson triplet,
             and a bulk Randall-Sundrum model with a heavy spin-2
             graviton. Cross-section limits are set at the 95% confidence
             level and are compared to theoretical cross-section
             predictions for a variety of models. The data exclude a
             scalar singlet with mass below 2650 GeV, a heavy
             vector-boson triplet with mass below 2600 GeV, and a
             graviton with mass below 1100 GeV. These results
             significantly extend the previous limits set using pp
             collisions at s=8 TeV.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP09(2016)173},
   Key = {fds321097}
}

@article{fds310329,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Searches for heavy long-lived charged particles with the
             ATLAS detector in proton-proton collisions at √s = 8
             Tev},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2015)068},
   Abstract = {Abstract: Searches for heavy long-lived charged particles
             are performed using a data sample of 19.1 fb−1 from
             proton-proton collisions at a centre-of-mass energy of s=8$$
             \sqrt{s}=8 $$ TeV collected by the ATLAS detector at the
             Large Hadron Collider. No excess is observed above the
             estimated background and limits are placed on the mass of
             long-lived particles in various supersymmetric models.
             Long-lived tau sleptons in models with gauge-mediated
             symmetry breaking are excluded up to masses between 440 and
             385 GeV for tan β between 10 and 50, with a 290 GeV limit
             in the case where only direct tau slepton production is
             considered. In the context of simplified LeptoSUSY models,
             where sleptons are stable and have a mass of 300 GeV, squark
             and gluino masses are excluded up to a mass of 1500 and 1360
             GeV, respectively. Directly produced charginos, in
             simplified models where they are nearly degenerate to the
             lightest neutralino, are excluded up to a mass of 620 GeV.
             R-hadrons, composites containing a gluino, bottom squark or
             top squark, are excluded up to a mass of 1270, 845 and 900
             GeV, respectively, using the full detector; and up to a mass
             of 1260, 835 and 870 GeV using an approach disregarding
             information from the muon spectrometer.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP01(2015)068},
   Key = {fds310329}
}

@article{fds356790,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Searches for heavy long-lived sleptons and R-hadrons with
             the ATLAS detector in pp collisions at √s=7
             TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {720},
   Number = {4-5},
   Pages = {277-308},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.02.015},
   Abstract = {A search for long-lived particles is performed using a data
             sample of 4.7 fb−1 from proton–proton collisions at a
             centre-of-mass energy s=7 TeV collected by the ATLAS
             detector at the LHC. No excess is observed above the
             estimated background and lower limits, at 95% confidence
             level, are set on the mass of the long-lived particles in
             different scenarios, based on their possible interactions in
             the inner detector, the calorimeters and the muon
             spectrometer. Long-lived staus in gauge-mediated
             SUSY-breaking models are excluded up to a mass of 300 GeV
             for tanβ=5–20. Directly produced long-lived sleptons are
             excluded up to a mass of 278 GeV. R-hadrons, composites of
             gluino (stop, sbottom) and light quarks, are excluded up to
             a mass of 985 GeV (683 GeV, 612 GeV) when using a generic
             interaction model. Additionally two sets of limits on
             R-hadrons are obtained that are less sensitive to the
             interaction model for R-hadrons. One set of limits is
             obtained using only the inner detector and calorimeter
             observables, and a second set of limits is obtained based on
             the inner detector alone.},
   Doi = {10.1016/j.physletb.2013.02.015},
   Key = {fds356790}
}

@article{fds356692,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Searches for heavy ZZ and ZW resonances in the ℓℓqq and
             ννqq final states in pp collisions at √s=13 TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2018},
   Number = {3},
   Year = {2018},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2018)009},
   Abstract = {This paper reports searches for heavy resonances decaying
             into ZZ or ZW using data from proton-proton collisions at a
             centre-of-mass energy of s=13 TeV. The data, corresponding
             to an integrated luminosity of 36.1 fb−1, were recorded
             with the ATLAS detector in 2015 and 2016 at the Large Hadron
             Collider. The searches are performed in final states in
             which one Z boson decays into either a pair of light charged
             leptons (electrons and muons) or a pair of neutrinos, and
             the associated W boson or the other Z boson decays
             hadronically. No evidence of the production of heavy
             resonances is observed. Upper bounds on the production cross
             sections of heavy resonances times their decay branching
             ratios to ZZ or ZW are derived in the mass range 300-5000GeV
             within the context of Standard Model extensions with
             additional Higgs bosons, a heavy vector triplet or warped
             extra dimensions. Production through gluon-gluon fusion,
             Drell-Yan or vector-boson fusion are considered, depending
             on the assumed model.[Figure not available: see
             fulltext.].},
   Doi = {10.1007/JHEP03(2018)009},
   Key = {fds356692}
}

@article{fds356544,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
             B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
             M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
             A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
             Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
             Pereira, R},
   Title = {Searches for lepton-flavour-violating decays of the Higgs
             boson in s=13 TeV pp collisions with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {800},
   Year = {2020},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.135069},
   Abstract = {This Letter presents direct searches for lepton flavour
             violation in Higgs boson decays, H→eτ and H→μτ,
             performed with the ATLAS detector at the LHC. The searches
             are based on a data sample of proton–proton collisions at
             a centre-of-mass energy s=13 TeV, corresponding to an
             integrated luminosity of 36.1 fb−1. No significant excess
             is observed above the expected background from Standard
             Model processes. The observed (median expected) 95%
             confidence-level upper limits on the lepton-flavour-violating
             branching ratios are 0.47% (0.34−0.10+0.13%) and 0.28%
             (0.37−0.10+0.14%) for H→eτ and H→μτ,
             respectively.},
   Doi = {10.1016/j.physletb.2019.135069},
   Key = {fds356544}
}

@article{fds372389,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
             SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
             AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
             A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
             MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce,
             ATH},
   Title = {Searches for new phenomena in events with two leptons, jets,
             and missing transverse momentum in 139 fb - 1 of
             √s=13 TeV pp collisions with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {6},
   Year = {2023},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11434-w},
   Abstract = {Searches for new phenomena inspired by supersymmetry in
             final states containing an e+e- or μ+μ- pair, jets, and
             missing transverse momentum are presented. These searches
             make use of proton–proton collision data with an
             integrated luminosity of 139fb-1 , collected during
             2015–2018 at a centre-of-mass energy s=13 TeV by the ATLAS
             detector at the Large Hadron Collider. Two searches target
             the pair production of charginos and neutralinos. One uses
             the recursive-jigsaw reconstruction technique to follow up
             on excesses observed in 36.1fb-1 of data, and the other uses
             conventional event variables. The third search targets pair
             production of coloured supersymmetric particles (squarks or
             gluinos) decaying through the next-to-lightest neutralino
             (χ~20) via a slepton (ℓ~) or Z boson into ℓ+ℓ-χ~10 ,
             resulting in a kinematic endpoint or peak in the dilepton
             invariant mass spectrum. The data are found to be consistent
             with the Standard Model expectations. Results are
             interpreted using simplified models and exclude masses up to
             900 GeV for electroweakinos, 1550 GeV for squarks, and
             2250 GeV for gluinos.},
   Doi = {10.1140/epjc/s10052-023-11434-w},
   Key = {fds372389}
}

@article{fds356578,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
             Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
             Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
             FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
             LJ and Armstrong, A and Arnaez, O},
   Title = {Searches for scalar leptoquarks and differential
             cross-section measurements in dilepton–dijet events in
             proton–proton collisions at a centre-of-mass energy of
             √s = 13 TeV with the ATLAS experiment},
   Journal = {European Physical Journal C},
   Volume = {79},
   Number = {9},
   Year = {2019},
   Month = {September},
   url = {http://dx.doi.org/10.1140/epjc/s10052-019-7181-x},
   Abstract = {Searches for scalar leptoquarks pair-produced in
             proton–proton collisions at s=13 TeV at the Large Hadron
             Collider are performed by the ATLAS experiment. A data set
             corresponding to an integrated luminosity of 36.1 fb- 1 is
             used. Final states containing two electrons or two muons and
             two or more jets are studied, as are states with one
             electron or muon, missing transverse momentum and two or
             more jets. No statistically significant excess above the
             Standard Model expectation is observed. The observed and
             expected lower limits on the leptoquark mass at 95%
             confidence level extend up to 1.29 TeV and 1.23 TeV for
             first- and second-generation leptoquarks, respectively, as
             postulated in the minimal Buchmüller–Rückl–Wyler
             model, assuming a branching ratio into a charged lepton and
             a quark of 50%. In addition, measurements of particle-level
             fiducial and differential cross sections are presented for
             the Z→ ee, Z→ μμ and tt¯ processes in several regions
             related to the search control regions. Predictions from a
             range of generators are compared with the measurements, and
             good agreement is seen for many of the observables. However,
             the predictions for the Z→ ℓℓ measurements in
             observables sensitive to jet energies disagree with the
             data.},
   Doi = {10.1140/epjc/s10052-019-7181-x},
   Key = {fds356578}
}

@article{fds321130,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
             A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and CabreraUrbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace,
             N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP},
   Title = {Searches for scalar leptoquarks in pp collisions at
             [Formula: see text] = 8 TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {5},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3823-9},
   Abstract = {Searches for pair-produced scalar leptoquarks are performed
             using 20 fb[Formula: see text] of proton-proton collision
             data provided by the LHC and recorded by the ATLAS detector
             at [Formula: see text] TeV. Events with two electrons
             (muons) and two or more jets in the final state are used to
             search for first (second)-generation leptoquarks. The
             results from two previously published ATLAS analyses are
             interpreted in terms of third-generation leptoquarks
             decaying to [Formula: see text] and [Formula: see text]
             final states. No statistically significant excess above the
             Standard Model expectation is observed in any channel and
             scalar leptoquarks are excluded at 95 % CL with masses up
             to [Formula: see text] 1050 GeV for first-generation
             leptoquarks, [Formula: see text] 1000 GeV for
             second-generation leptoquarks, [Formula: see text] 625 GeV
             for third-generation leptoquarks in the [Formula: see
             text] channel, and 200 [Formula: see text] 640 GeV in
             the [Formula: see text] channel.},
   Doi = {10.1140/epjc/s10052-015-3823-9},
   Key = {fds321130}
}

@article{fds307760,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Searches for supersymmetry with the ATLAS detector using
             final states with two leptons and missing transverse
             momentum in s=7TeV proton-proton collisions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {709},
   Number = {3},
   Pages = {137-157},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.01.076},
   Abstract = {Results of three searches are presented for the production
             of supersymmetric particles decaying into final states with
             missing transverse momentum and exactly two isolated
             leptons, e or μ. The analysis uses a data sample collected
             during the first half of 2011 that corresponds to a total
             integrated luminosity of 1fb-1 of s=7TeV proton-proton
             collisions recorded with the ATLAS detector at the Large
             Hadron Collider. Opposite-sign and same-sign dilepton events
             are separately studied, with no deviations from the Standard
             Model expectation observed. Additionally, in opposite-sign
             events, a search is made for an excess of same-flavour over
             different-flavour lepton pairs. Effective production cross
             sections in excess of 9.9 fb for opposite-sign events
             containing supersymmetric particles with missing transverse
             momentum greater than 250 GeV are excluded at 95% CL. For
             same-sign events containing supersymmetric particles with
             missing transverse momentum greater than 100 GeV, effective
             production cross sections in excess of 14.8 fb are excluded
             at 95% CL. The latter limit is interpreted in a simplified
             electroweak gaugino production model excluding chargino
             masses up to 200 GeV, under the assumption that slepton
             decay is dominant. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.01.076},
   Key = {fds307760}
}

@article{fds307579,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bertoli, G and Bhatti, A and Bland, KR and Blumenfeld,
             B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
             A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
             F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo,
             S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci, MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina,
             K},
   Title = {Searches for the Higgs boson decaying to W+W
             -→ℓ+νℓ-ν̄ with the
             CDF II detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.052012},
   Abstract = {We present a search for a standard model Higgs boson
             decaying to two W bosons that decay to leptons using the
             full data set collected with the CDF II detector in
             √s=1.96 TeV pp̄ collisions at the Fermilab Tevatron,
             corresponding to an integrated luminosity of 9.7 fb-1. We
             obtain no evidence for production of a standard model Higgs
             boson with mass between 110 and 200 GeV/c2, and place upper
             limits on the production cross section within this range. We
             exclude standard model Higgs boson production at the 95%
             confidence level in the mass range between 149 and 172
             GeV/c2, while expecting to exclude, in the absence of
             signal, the range between 155 and 175 GeV/c2. We also
             interpret the search in terms of standard model Higgs boson
             production in the presence of a fourth generation of
             fermions and within the context of a fermiophobic Higgs
             boson model. For the specific case of a standard-model-like
             Higgs boson in the presence of fourth-generation fermions,
             we exclude at the 95% confidence level Higgs boson
             production in the mass range between 124 and 200 GeV/c2,
             while expecting to exclude, in the absence of signal, the
             range between 124 and 221 GeV/c2. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.88.052012},
   Key = {fds307579}
}

@article{fds356731,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Searches for the Zγ decay mode of the Higgs boson and for
             new high-mass resonances in pp collisions at √s=13 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {10},
   Year = {2017},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2017)112},
   Abstract = {This article presents searches for the Zγ decay of the
             Higgs boson and for narrow high-mass resonances decaying to
             Zγ, exploiting Z boson decays to pairs of electrons or
             muons. The data analysis uses 36.1 fb−1 of pp collisions
             at s=13 recorded by the ATLAS detector at the CERN Large
             Hadron Collider. The data are found to be consistent with
             the expected Standard Model background. The observed
             (expected — assuming Standard Model pp → H → Zγ
             production and decay) upper limit on the production cross
             section times the branching ratio for pp → H → Zγ is
             6.6. (5.2) times the Standard Model prediction at the 95%
             confidence level for a Higgs boson mass of 125.09 GeV. In
             addition, upper limits are set on the production cross
             section times the branching ratio as a function of the mass
             of a narrow resonance between 250 GeV and 2.4 TeV, assuming
             spin-0 resonances produced via gluon-gluon fusion, and
             spin-2 resonances produced via gluon-gluon or
             quark-antiquark initial states. For high-mass spin-0
             resonances, the observed (expected) limits vary between 88
             fb (61 fb) and 2.8 fb (2.7 fb) for the mass range from 250
             GeV to 2.4 TeV at the 95% confidence level.},
   Doi = {10.1007/JHEP10(2017)112},
   Key = {fds356731}
}

@article{fds356595,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger,
             M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou,
             C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Arduh, FA and Arguin, JF},
   Title = {Searches for third-generation scalar leptoquarks in √s =
             13 TeV pp collisions with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {6},
   Year = {2019},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2019)144},
   Abstract = {Limits are set on the pair production of scalar leptoquarks,
             where all possible decays of the leptoquark into a quark (t,
             b) and a lepton (τ, ν) of the third generation are
             considered. The limits are presented as a function of the
             leptoquark mass and the branching ratio into charged leptons
             for up-type (LQ3u → tν/bτ) and down-type (LQ3d →
             bν/tτ) leptoquarks. Many results are reinterpretations of
             previously published ATLAS searches. In all cases, LHC
             proton-proton collision data at a centre-of-mass energy of s
             = 13 TeV recorded by the ATLAS detector in 2015 and 2016 are
             used, corresponding to an integrated luminosity of 36.1
             fb−1. Masses below 800 GeV are excluded for both LQ3u and
             LQ3d independently of the branching ratio, with masses below
             about 1 TeV being excluded for the limiting cases of
             branching ratios equal to zero or unity.[Figure not
             available: see fulltext.].},
   Doi = {10.1007/JHEP06(2019)144},
   Key = {fds356595}
}

@article{fds359268,
   Author = {Kotwal, AV},
   Title = {Searching for metastable particles using graph
             computing.},
   Journal = {Scientific reports},
   Volume = {11},
   Number = {1},
   Pages = {18543},
   Year = {2021},
   Month = {September},
   url = {http://dx.doi.org/10.1038/s41598-021-97848-6},
   Abstract = {The reconstruction of charged particle trajectories at the
             Large Hadron Collider and future colliders relies on energy
             depositions in sensors placed at distances ranging from a
             centimeter to a meter from the colliding beams. We propose a
             method of detecting charged particles that decay invisibly
             after traversing a short distance of about 25 cm inside the
             experimental apparatus. One of the decay products may
             constitute the dark matter known to be 84% of all matter at
             galactic and cosmological distance scales. Our method uses
             graph computing to cluster spacepoints recorded by
             two-dimensional silicon pixel sensors into
             mathematically-defined patterns. The algorithm may be
             implemented on silicon-based integrated circuits using
             field-programmable gate array technology to augment or
             replace traditional computing platforms.},
   Doi = {10.1038/s41598-021-97848-6},
   Key = {fds359268}
}

@article{fds307986,
   Author = {Aaltonen, T and others},
   Title = {Searching the inclusive ℓγE̸T+b-quark signature for
             radiative top quark decay and non-standard-model
             processes},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {1},
   Pages = {011102},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.011102},
   Abstract = {We compare the inclusive production of events containing a
             lepton (ℓ), a photon (γ), significant transverse momentum
             imbalance (E̸T), and a jet identified as containing a
             b-quark, to SM predictions. The search uses data produced in
             proton-antiproton collisions at sqrt[s]=1.96  TeV
             corresponding to 1.9  fb-1 of integrated luminosity
             taken with the CDF detector. We find 28 ℓγbE̸T events
             versus an expectation of 31.0-3.5+4.1 events. If we further
             require events to contain at least three jets and large
             total transverse energy, the largest SM source is radiative
             top-quark pair production, tt̅ +γ. In the data we observe
             16 tt̅ γ candidate events versus an expectation from SM
             sources of 11.2-2.1+2.3. Assuming the difference between the
             observed number and the predicted non-top-quark total of
             6.8-2.0+2.2 is due to SM top-quark production, we estimate
             the tt̅ γ cross section to be 0.15 &plusmn;
             0.08  pb.},
   Doi = {10.1103/PhysRevD.80.011102},
   Key = {fds307986}
}

@article{fds310307,
   Author = {Auerbach, B and Chekanov, S and Love, J and Proudfoot, J and Kotwal,
             AV},
   Title = {Sensitivity to new high-mass states decaying to tt¯ at a
             100 TeV collider},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.034014},
   Abstract = {We discuss the sensitivity of a 100 TeV pp collider to heavy
             particles decaying to top-antitop (tt¯) final states. This
             center-of-mass energy, together with an integrated
             luminosity of 10ab-1, can produce heavy particles in the
             mass range of several tens of teraelectronvolts (TeV). A
             Monte Carlo study is performed using boosted-top techniques
             to reduce QCD background for the reconstruction of heavy
             particles with masses in the range of 8-20 TeV, and various
             widths. In particular, we study two models that predict
             heavy states, a model with an extra gauge boson (Z0′) and
             with a Kaluza-Klein (KK) excitation of the gluon (gKK). We
             estimate the sensitive values of σ×Br of about 2 (4) fb
             for Z0′ (gKK), with a corresponding mass reach of 13 (20)
             TeV.},
   Doi = {10.1103/PhysRevD.91.034014},
   Key = {fds310307}
}

@article{fds346201,
   Author = {Singh, M and Kotwal, A and Gupta, RM and Adhya, S and Chatterjee, K and Jayaram, J},
   Title = {Sero-Epidemiological and Behavioural Survey of HIV, HBV and
             HCV amongst Indian Armed Forces Trainees.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {66},
   Number = {1},
   Pages = {50-54},
   Year = {2010},
   Month = {January},
   url = {http://dx.doi.org/10.1016/s0377-1237(10)80093-0},
   Abstract = {<h4>Background</h4>Information on the emerging epidemics of
             Human immunodeficiency virus (HIV), Hepatitis B (HBV) and C
             (HCV) viruses in younger age groups in India is scanty due
             to paucity of representative, population based surveys and
             varied estimation methodology. This study was done to assess
             the point prevalence of HIV, HBV and HCV infections
             alongwith the epidemiological factors associated with these
             infections. Attitudes, beliefs and behaviour related to
             sexual and injecting drug practices, with a view to assess
             the need for introduction of screening program for the new
             entrants of the armed forces was also studied.<h4>Methods</h4>A
             multi-centric cross sectional serological and behavioural
             survey was carried out amongst newly enrolled trainees of
             the Armed Forces in 2004. The group was selected by
             multistage random sampling giving equal representation to
             all regions of India. Study subjects were interviewed using
             a pretested, validated questionnaire and screened for HIV,
             HBV and HCV infections by rapid tests. Standard confirmatory
             tests were carried out for trainees testing positive.
             Quality assurance measures were integral part of each
             activity. A database was created in MS Access and SPSS ver
             11.0.1 was used for analysis.<h4>Result</h4>Out of the
             23,000 trainees included in the study, 22666 (98.55%) were
             included in the analysis. The age, formal education and age
             at first sexual intercourse of participants ranged from
             16-25 years (median 20), 8-17 years (median 10) and 12-25
             years, respectively. Partial knowledge about routes of
             spread of HIV was highly prevalent but complete knowledge
             was extremely low. Per thousand point prevalence of HIV, HBV
             and HCV was 0.61 (95% CI, 0.34-10.3, poisson), 9.31
             (8.1-10.65) and 4.44 (3.61-5.39), respectively. Clustering
             of HIV (4.56 per 1000, 2.19-8.38) and HCV (30.54 per 1000,
             23.67-38.78) and a higher number of HCV as compared to HBV
             was found amongst trainees from northeast. A statistically
             significant association was found between history of
             injecting drug use (other than medical) and HCV
             (p<0.05).<h4>Conclusion</h4>Self-exclusion for recruitment
             as military trainees might have resulted in underestimation
             of general population figures but results provide region
             wise estimates unavailable till now. Concerted efforts are
             required in the current HIV/AIDS program activities to bring
             about knowledge and behaviour change amongst teenagers and
             young adults.},
   Doi = {10.1016/s0377-1237(10)80093-0},
   Key = {fds346201}
}

@article{fds346180,
   Author = {Kumar, S and Gupta, RM and Sen, S and Sarkar, RS and Philip, J and Kotwal,
             A and Sumathi, SH},
   Title = {Seroprevalence of human parvovirus B19 in healthy blood
             donors.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {69},
   Number = {3},
   Pages = {268-272},
   Year = {2013},
   Month = {July},
   url = {http://dx.doi.org/10.1016/j.mjafi.2012.11.009},
   Abstract = {<h4>Background</h4>Human parvovirus B19 is an emerging
             transfusion transmitted infection. Although parvovirus B19
             infection is connected with severe complications in some
             recipients, donor screening is not yet mandatory. To reduce
             the risk of contamination, plasma-pool screening and
             exclusion of highly viraemic donations are recommended. In
             this study the prevalence of parvovirus B19 in healthy blood
             donors was detected by ELISA.<h4>Methods</h4>A total of 1633
             samples were screened for IgM and IgG antibodies against
             parvovirus B19 by ELISA. The initial 540 samples were
             screened for both IgM and IgG class antibodies and remaining
             1093 samples were screened for only IgM class antibodies by
             ELISA.<h4>Results</h4>Net prevalence of IgM antibodies to
             human parvovirus B19 in our study was 7.53% and prevalence
             of IgG antibodies was 27.96%. Dual positivity (IgG and IgM)
             was 2.40%.<h4>Conclusion</h4>The seroprevalence of human
             parvovirus B19 among blood donor population in our study is
             high, and poses an adverse transfusion risk especially in
             high-risk group of patients who have no detectable
             antibodies to B19. Studies with large sample size are needed
             to validate these results.},
   Doi = {10.1016/j.mjafi.2012.11.009},
   Key = {fds346180}
}

@article{fds347531,
   Author = {Kotwal, A and Cutrona, SL},
   Title = {Serotonin Syndrome in the Setting of Lamotrigine,
             Aripiprazole, and Cocaine Use.},
   Journal = {Case reports in medicine},
   Volume = {2015},
   Pages = {769531},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1155/2015/769531},
   Abstract = {Serotonin syndrome is a potentially life-threatening
             condition associated with increased serotonergic activity in
             the central nervous system. It is classically associated
             with the simultaneous administration of two serotonergic
             agents, but it can occur after initiation of a single
             serotonergic drug or increasing the dose of a serotonergic
             drug in individuals who are particularly sensitive to
             serotonin. We describe a case of serotonin syndrome that
             occurred after ingestion of higher than prescribed doses of
             lamotrigine and aripiprazole, in addition to cocaine abuse.
             The diagnosis was established based on Hunter toxicity
             criteria and severity was classified as mild. The features
             of this syndrome resolved shortly after discontinuation of
             the offending agents. Serotonin syndrome is characterized by
             mental status changes, autonomic hyperactivity, and
             neuromuscular abnormalities along a spectrum ranging from
             mild to severe. Serotonin syndrome in our patient was most
             likely caused by the pharmacokinetic and pharmacodynamic
             interactions between lamotrigine, aripiprazole, and cocaine
             leading to increased CNS serotonergic activity.},
   Doi = {10.1155/2015/769531},
   Key = {fds347531}
}

@booklet{Adams95,
   Author = {Adams, MR and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Breidung, H and Busza, W and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dhawan, SK and Dietrich, FS and Dougherty,
             W and Dreyer, T and Eckardt, V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen,
             KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Hughes, VW and Jackson, HE and Jaffe, DE and Jancso, G and Jansen, DM and Jin, Z and Kaufman, S and Kennedy, RD and Kinney, ER and Kirk, T and Kobrak, HGE and Kotwal, AV and Kunori, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin, JG and Nickerson, RB and Novak, J and O'Day, S and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou, V and Pawlik, B and Pipkin, FM and Potterveld, DH and Ramberg, EJ and Röser, A and Ryan, JJ and Salgado, CW and Salvarani, A and Schellman, H and Schmitt, M and Schmitz, N and Schüler, KP and Siegert,
             G and Skuja, A and Snow, GA and Söldner-Rembold, S and Spentzouris, P and Stier, HE and Stopa, P and Swanson, RA and Venkataramania, H and Wilhelm, M and Wilson, R and Wittek, W and Wolbers, SA and Zghiche, A and Zhao, T},
   Title = {Shadowing in inelastic scattering of muons on carbon,
             calcium and lead at low xBj},
   Journal = {Zeitschrift für Physik C Particles and Fields},
   Volume = {67},
   Number = {3},
   Pages = {403-410},
   Publisher = {Springer Nature},
   Year = {1995},
   Month = {September},
   url = {http://dx.doi.org/10.1007/BF01624583},
   Abstract = {Nuclear shadowing is observed in the per-nucleon cross
             sections of positive muons on carbon, calcium and lead as
             compared to deuterium. The data were taken by Fermilab
             experiment E665 using inelastically scattered muons of mean
             incident momentum 470 GeV/c. Cross-section ratios are
             presented in the kinematic region 0.0001<xBj<0.56 and
             0.1<Q2<80 GeV2. The data are consistent with no significant
             ν or Q2 dependence at fixed xBj. As xBj decreases, the size
             of the shadowing effect, as well as its A dependence, are
             found to approach the corresponding measurements in
             photoproduction. © 1995 Springer-Verlag.},
   Doi = {10.1007/BF01624583},
   Key = {Adams95}
}

@article{fds307584,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Signature-based search for delayed photons in exclusive
             photon plus missing transverse energy events from pp̄
             collisions with √s=1.96 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {3},
   Pages = {031103},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.031103},
   Abstract = {We present the first signature-based search for delayed
             photons using an exclusive photon plus missing transverse
             energy final state. Events are reconstructed in a data
             sample from the CDF II detector corresponding to 6.3 fb-1 of
             integrated luminosity from √s=1.96 TeV proton-antiproton
             collisions. Candidate events are selected if they contain a
             photon with an arrival time in the detector larger than
             expected from a promptly produced photon. The mean number of
             events from standard model sources predicted by the
             data-driven background model based on the photon timing
             distribution is 286±24. A total of 322 events are observed.
             A p value of 12% is obtained, showing consistency of the
             data with standard model predictions. © 2013 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.88.031103},
   Key = {fds307584}
}

@article{fds310297,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Simultaneous measurements of the tt¯, W+W-, and Z/γ∗
             →ττ production cross-sections in pp collisions at √s
             =7 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.052005},
   Abstract = {Simultaneous measurements of the tt¯, W+W-, and
             Z/γ∗→ττ production cross-sections using an integrated
             luminosity of 4.6 fb-1 of pp collisions at √s=7 TeV
             collected by the ATLAS detector at the LHC are presented.
             Events are selected with two high transverse momentum
             leptons consisting of an oppositely charged electron and
             muon pair. The three processes are separated using the
             distributions of the missing transverse momentum of events
             with zero and greater than zero jet multiplicities.
             Measurements of the fiducial cross-section are presented
             along with results that quantify for the first time the
             underlying correlations in the predicted and measured
             cross-sections due to proton parton distribution functions.
             These results indicate that the correlated
             next-to-leading-order predictions for tt¯ and
             Z/γ∗→ττ underestimate the data, while those at
             next-to-next-to-leading-order generally describe the data
             well. The full cross-sections are measured to be
             σ(tt¯)=181.2±2.8-9.5+9.7±3.3±3.3 pb,
             σ(W+W-)=53.3±2.7-8.0+7.3±1.0±0.5 pb, and
             σ(Z/γ∗→ττ)=1174±24-87+72±21±9 pb, where the cited
             uncertainties are due to statistics, systematic effects,
             luminosity and the LHC beam energy measurement,
             respectively. The W+W- measurement includes the small
             contribution from Higgs boson decays, H→W+W-.},
   Doi = {10.1103/PhysRevD.91.052005},
   Key = {fds310297}
}

@article{fds307620,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M and Armbruster, AJ and Arnaez, O},
   Title = {Single hadron response measurement and calorimeter jet
             energy scale uncertainty with the ATLAS detector at the
             LHC},
   Journal = {European Physical Journal C},
   Volume = {73},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2305-1},
   Abstract = {The uncertainty on the calorimeter energy response to jets
             of particles is derived for the ATLAS experiment at the
             Large Hadron Collider (LHC). First, the calorimeter response
             to single isolated charged hadrons is measured and compared
             to the Monte Carlo simulation using proton-proton collisions
             at centre-of-mass energies of √s = 900 GeV and 7 TeV
             collected during 2009 and 2010. Then, using the decay of
             K<inf>s</inf> and Λ particles, the calorimeter response to
             specific types of particles (positively and negatively
             charged pions, protons, and anti-protons) is measured and
             compared to the Monte Carlo predictions. Finally, the jet
             energy scale uncertainty is determined by propagating the
             response uncertainty for single charged and neutral
             particles to jets. The response uncertainty is 2–5 % for
             central isolated hadrons and 1–3 % for the final
             calorimeter jet energy scale.},
   Doi = {10.1140/epjc/s10052-013-2305-1},
   Key = {fds307620}
}

@article{fds322004,
   Author = {Kotwal, AV and Ramsey-Musolf, MJ and No, JM and Winslow,
             P},
   Title = {Singlet-catalyzed electroweak phase transitions in the 100
             TeV frontier SINGLET-CATALYZED ELECTROWEAK PHASE ... KOTWAL
             et al.},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.035022},
   Abstract = {We study the prospects for probing a gauge singlet
             scalar-driven strong first-order electroweak phase
             transition with a future proton-proton collider in the 100
             TeV range. Singlet-Higgs mixing enables resonantly enhanced
             di-Higgs production, potentially aiding discovery prospects.
             We perform Monte Carlo scans of the parameter space to
             identify regions associated with a strong first-order
             electroweak phase transition, analyze the corresponding
             di-Higgs signal, and select a set of benchmark points that
             span the range of di-Higgs signal strengths. For the bbγγ
             and 4τ final states, we investigate discovery prospects for
             each benchmark point for the high-luminosity phase of the
             Large Hadron Collider and for a future pp collider with
             s=50, 100, or 200 TeV. We find that any of these future
             collider scenarios could significantly extend the reach
             beyond that of the high-luminosity LHC, and that with s=100
             TeV (200 TeV) and 30 ab-1, the full region of parameter
             space favorable to strong first-order electroweak phase
             transitions is almost fully (fully) discoverable.},
   Doi = {10.1103/PhysRevD.94.035022},
   Key = {fds322004}
}

@article{fds308211,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Balamurali, V and Baldin, B and Banerjee,
             S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding,
             F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey,
             D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang,
             SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
             AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger,
             C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
             P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
             G},
   Title = {Small angle J/ψ production in pp¯ collisions at
             √s=1.8TeV},
   Journal = {Physical Review Letters},
   Volume = {82},
   Number = {1},
   Pages = {35-40},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.82.35},
   Abstract = {This paper presents the first measurement of inclusive J/ψ
             production cross section in the forward pseudorapidity
             region 2.5≤|ηJ/ψ|≤3.7 in pp¯ collisions at √S=1.8
             TeV. The results are based on 9.8 pb−1 of data collected
             using the D0 detector at the Fermilab Tevatron Collider. The
             inclusive J/ψ cross section for transverse momenta between
             1 and 16 GeV/c is compared with theoretical models of
             charmonium production. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.82.35},
   Key = {fds308211}
}

@article{fds308199,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
             JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
             M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and del
             Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
             HT and Diesburg, M and di Loreto, G and Draper, P and Ducros, Y and Dudko,
             LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
             VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
             OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Fatyga,
             MK and Feher, S and Fein, D and Ferbel, T},
   Title = {Small-angle muon and bottom-quark production in pp̄
             collisions at √s = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {84},
   Number = {24},
   Pages = {5478-5483},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevLett.84.5478},
   Abstract = {The inclusive muon cross section, and the cross section for
             mouns originating from b quark decay, in the forward
             rapidity region of 2.4 < | ymu | < 3.2 were measured in this
             study. It was found that next-to-leading order QCD
             calculations underestimate b quark production by a factor of
             4 in this region.},
   Doi = {10.1103/PhysRevLett.84.5478},
   Key = {fds308199}
}

@article{fds362574,
   Author = {Agashe, K and Erbacher, R and Gerber, CE and Melnikov, K and Schwienhorst, R and Mitov, A and Vos, M and Wimpenny, S and Adelman, J and Baumgart, M and Garcia-Bellido, A and Loginov, A and Jung, A and Schulze, M and Shelton, J and Craig, N and Velasco, M and Golling, T and Hubisz, J and Ivanov, A and Perelstein, M and Chekanov, S and Dolen, J and Pilot, J and Pöschl, R and Tweedie, B and Alioli, S and Alvarez-Gonzalez, B and Amidei, D and Andeen, T and Arce, A and Auerbach, B and Avetisyan, A and Backovic, M and Bai, Y and Begel, M and Berge, S and Bernard, C and Bernius, C and Bhattacharya, S and Black, K and Blondel, A and Bloom, K and Bose, T and Boudreau, J and Brau, J and Broggio, A and Brooijmans, G and Brost, E and Calkins, R and Chakraborty, D and Childress, T and Choudalakis, G and Coco, V and Conway, JS and Degrande, C and Delannoy, A and Deliot, F and Dell'Asta,
             L and Drueke, E and Dutta, B and Effron, A and Ellis, K and Erdmann, J and Evans, J and Feng, C and Feng, E and Ferroglia, A and Finelli, K and Flanagan, W and Fleck, I and Freitas, A and Garberson, F and Suarez, RG and Graesser, ML and Graf, N and Greenwood, Z and George, J and Group, C and Gurrola, A and Hammad, G and Han, T and Han, Z and Heintz, U and Hoeche, S and Horiguchi, T and Iashvili, I and Ismail, A and Jain, S and Janot, P and Johns, W and Joshi, J and Juste, A and Kamon, T and Kao, C and Kats, Y and Katz, A and Kaur, M and Kehoe, R and Keung, W and Khalil, S and Khanov, A and Kharchilava, A and Kidonakis, N and Kilic, C and Kolev, N and Kotwal, A and Kraus, J and Krohn, D and Kruse, M and Kumar, A and Lee, S and Luiggi, E and Mantry, S and Melo, A and Miller, D and Moortgat-Pick, G and Narain, M and Odell, N and Oksuzian, Y and Oreglia, M and Penin, A and Peters, Y and Pollard, C and Poss, S and Rappoccio, HBPS and Redford, S and Reece, M and Rizatdinova, F and Roloff, P and Ruiz, R and Saleem, M and Schoenrock,
             B and Schwanenberger, C and Schwarz, T and Seidel, K and Shabalina, E and Sheldon, P and Simon, F and Sinha, K and Skands, P and Skubik, P and Sterman, G and Stolarski, D and Strube, J and Stupak, J and Su, S and Tesar, M and Thomas, S and Thompson, E and Tipton, P and Varnes, E and Vignaroli, N and Virzi, J and Vogel, M and Walker, D and Wang, K and Webber, B and Wells, JD and Westhoff, S and Whiteson, D and Williams, M and Wu, S and Yang, U and Yokoya, H and Yoo, H and Zhang, H and Zhou, N and Zhu,
             H and Zupan, J},
   Title = {Snowmass 2013 Top quark working group report},
   Year = {2013},
   Month = {November},
   Abstract = {This report summarizes the work of the Energy Frontier Top
             Quark working group of the 2013 Community Summer Study
             (Snowmass).},
   Key = {fds362574}
}

@article{fds362578,
   Author = {Anderson, J and Avetisyan, A and Brock, R and Chekanov, S and Cohen, T and Dhingra, N and Dolen, J and Hirschauer, J and Howe, K and Kotwal, A and LeCompte, T and Malik, S and Mcbride, P and Mishra, K and Narain, M and Olsen, J and Padhi, S and Peskin, ME and III, JS and Wacker,
             JG},
   Title = {Snowmass Energy Frontier Simulations},
   Year = {2013},
   Month = {September},
   Abstract = {This document describes the simulation framework used in the
             Snowmass Energy Frontier studies for future Hadron
             Colliders. An overview of event generation with {\sc
             Madgraph}5 along with parton shower and hadronization with
             {\sc Pythia}6 is followed by a detailed description of
             pile-up and detector simulation with {\sc Delphes}3. Details
             of event generation are included in a companion paper cited
             within this paper. The input parametrization is chosen to
             reflect the best object performance expected from the future
             ATLAS and CMS experiments; this is referred to as the
             "Combined Snowmass Detector". We perform simulations of $pp$
             interactions at center-of-mass energies $\sqrt{s}=$ 14, 33,
             and 100 TeV with 0, 50, and 140 additional $pp$ pile-up
             interactions. The object performance with multi-TeV $pp$
             collisions are studied for the first time using large
             pile-up interactions.},
   Key = {fds362578}
}

@article{fds308207,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bean, A and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar,
             V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buescher,
             V and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum,
             Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev,
             SV and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
             K and De, K and del Signore, K and Demarteau, M and Denisov, D and Denisov,
             SP and Diehl, HT and Diesburg, M and di Loreto, G and Draper, P and Ducros,
             Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison,
             J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
             T and Feher, S and Fein, D and Ferbel, T},
   Title = {Spin correlation in tt̄ production from pp̄ collisions at
             √s = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {85},
   Number = {2},
   Pages = {256-261},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.85.256},
   Abstract = {An analytical study was carried out to account for spin
             correlation effects in the production of tt̄ pairs in pp̄
             collisions at √s=1.8 TeV. It was found that κ > -0.25 at
             the 68% confidence level.},
   Doi = {10.1103/PhysRevLett.85.256},
   Key = {fds308207}
}

@article{fds316845,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Standalone vertex finding in the ATLAS muon
             spectrometer},
   Journal = {Journal of Instrumentation},
   Volume = {9},
   Number = {2},
   Pages = {P02001-P02001},
   Publisher = {IOP Publishing},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1748-0221/9/02/P02001},
   Abstract = {A dedicated reconstruction algorithm to find decay vertices
             in the ATLAS muon spectrometer is presented. The algorithm
             searches the region just upstream of or inside the muon
             spectrometer volume for multi-particle vertices that
             originate from the decay of particles with long decay paths.
             The performance of the algorithm is evaluated using both a
             sample of simulated Higgs boson events, in which the Higgs
             boson decays to long-lived neutral particles that in turn
             decay to bb final states, and pp collision data at √s = 7
             TeV collected with the ATLAS detector at the LHC during
             2011.},
   Doi = {10.1088/1748-0221/9/02/P02001},
   Key = {fds316845}
}

@article{fds308158,
   Author = {Kotwal, A},
   Title = {Status and plans of the tevatron electroweak working
             group},
   Journal = {AIP Conference Proceedings},
   Volume = {753},
   Pages = {149-157},
   Publisher = {AIP},
   Year = {2005},
   Month = {March},
   url = {http://dx.doi.org/10.1063/1.1896697},
   Abstract = {The Tevatron Electroweak Working group was created in
             September, 2003 at Fermilab to consolidate electroweak
             physics results for precision Standard Model tests. It is
             the first combined analysis group at Fermilab to publish in
             a refereed journal. The group currently has 49 subscribers.
             Three subgroups are dedicated to studies of W and Z boson
             properties, top quark properties, and Higgs physics
             respectively. The group has produced combined results from
             the CDF and DØ experiments on the Run 1 W boson mass and
             width, the Run 1 top quark mass, and the Run 2 measurement
             of the ratio of W and Z boson cross sections. New results
             are anticipated as Run 2 analyses mature. The group also
             organizes joint workshops for theorists and
             experimentalists. © 2005 American Institute of
             Physics.},
   Doi = {10.1063/1.1896697},
   Key = {fds308158}
}

@article{fds346203,
   Author = {Roshan, A and Kotwal, A and Riaz, M and Stanley, PRW},
   Title = {Sternal wound dehiscence complicated by macromastia: report
             of two cases with discussion of literature.},
   Journal = {Journal of plastic, reconstructive & aesthetic surgery :
             JPRAS},
   Volume = {62},
   Number = {10},
   Pages = {e362-e364},
   Year = {2009},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.bjps.2008.02.019},
   Abstract = {Sternal wound dehiscence complicated by macromastia can be
             difficult to treat by standard musculocutaneous flaps alone.
             We present our experience with two cases of sternal wound
             dehiscence complicated by macromastia, and their subsequent
             healing with a combination of reduction mammoplasty and
             local musculocutaneous flaps. Reduction mammoplasty is a
             useful adjunctive procedure in patients with macromastia
             complicating sternal wound dehiscence.},
   Doi = {10.1016/j.bjps.2008.02.019},
   Key = {fds346203}
}

@article{fds346197,
   Author = {Sinha, A and Kushwaha, AS and Kotwal, A and Sanghi, S and Verma,
             AK},
   Title = {Stigma in leprosy: miles to go!},
   Journal = {Indian journal of leprosy},
   Volume = {82},
   Number = {3},
   Pages = {137-145},
   Year = {2010},
   Month = {July},
   Abstract = {No disease has been more closely associated with stigma than
             leprosy such that it has become a metaphor for stigma.
             Stigma has been difficult to measure and little research has
             been done on this issue. Stigma reduction has not been an
             important component of anti-leprosy program. The study was
             undertaken to measure the stigma associated with leprosy by
             using P scale which is used for assessing participation
             restriction of those affected by the disease. This
             comparative questionnaire based study was carried out in two
             sets of patients. Two groups of 30 patients each were
             studied. First group belonged to a Government run
             Leprosarium and group two from a tertiary care skin and
             leprosy centre. The study used the Participation (P) scale
             and data was collected by interviewing the patients.
             Participation restriction was defined as any score equal to
             and more than 13. Participation restriction was observed in
             27 (90%) cases of group 1while participation restriction was
             present in only 7 (23.3%) subjects of group 2. It was
             observed that mean score of participation restriction in
             group 1 was quite high at 31.9 while it was only 8.3 for
             group 2. The participation restriction was directly related
             to the duration of disease and the grade of disability.
             Longer the duration of disease, greater was the likelihood
             of restriction. The participation restriction was found to
             be negatively correlated with the education. Recommendation
             about prevention of disability would require program about
             early diagnosis of nerve damage and subsequent action at the
             patient-family-community level and health care
             providers.},
   Key = {fds346197}
}

@article{fds346217,
   Author = {Seth, R and Kotwal, A and Ganguly, KK},
   Title = {Street and working children of Delhi, India, misusing
             toluene: an ethnographic exploration.},
   Journal = {Substance use & misuse},
   Volume = {40},
   Number = {11},
   Pages = {1659-1679},
   Year = {2005},
   Month = {January},
   url = {http://dx.doi.org/10.1080/10826080500222792},
   Abstract = {Our qualitative study explored: the perceptions of street
             children indulging in whitener fluid misuse; the social,
             economic, and cultural determinants of use; and users' views
             regarding effective preventive and control strategies.
             Forty-five in-depth interviews and three focus group
             discussions were conducted between March and December 2003.
             A purposive sample of those working children who were using
             toluene was selected by Snowball sampling. The paper
             discusses the: determinants of initiation and continued use;
             drug user social networks; psycho emotional deprivation and
             frustrations of these children; socio-cultural aspects like
             work driven need; others' attitudinal response towards them
             and their work; parental support or the lack of it; and
             strategies for prevention of this misuse.},
   Doi = {10.1080/10826080500222792},
   Key = {fds346217}
}

@article{fds372604,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
             Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
             JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
             M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends,
             KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira,
             MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos,
             P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat,
             A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley,
             JR and Batool, B and Battaglia, M and Bauce, M and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
             P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov,
             VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
             M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer,
             JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi,
             G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya,
             DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel,
             O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul,
             A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird,
             GA and Birman, M and Bisanz, T and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal,
             J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
             JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner,
             L and Brenner, R and Bressler, S and Brickwedde, B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
             EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
             AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
             Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo
             Garcia, L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi,
             E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen,
             SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
             G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov,
             MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
             BM and Clark, A and Clark, PJ and Clavijo Columbie and JM and Clawson, SE and Clement, C},
   Title = {Strong Constraints on Jet Quenching in Centrality-Dependent
             p+Pb Collisions at 5.02 TeV from ATLAS.},
   Journal = {Physical review letters},
   Volume = {131},
   Number = {7},
   Pages = {072301},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.131.072301},
   Abstract = {Jet quenching is the process of color-charged partons losing
             energy via interactions with quark-gluon plasma droplets
             created in heavy-ion collisions. The collective expansion of
             such droplets is well described by viscous hydrodynamics.
             Similar evidence of collectivity is consistently observed in
             smaller collision systems, including pp and p+Pb collisions.
             In contrast, while jet quenching is observed in Pb+Pb
             collisions, no evidence has been found in these small
             systems to date, raising fundamental questions about the
             nature of the system created in these collisions. The ATLAS
             experiment at the Large Hadron Collider has measured the
             yield of charged hadrons correlated with reconstructed jets
             in 0.36  nb^{-1} of p+Pb and 3.6  pb^{-1} of pp
             collisions at 5.02 TeV. The yields of charged hadrons with
             p_{T}^{ch}>0.5  GeV near and opposite in azimuth to jets
             with p_{T}^{jet}>30 or 60 GeV, and the ratios of these
             yields between p+Pb and pp collisions, I_{pPb}, are
             reported. The collision centrality of p+Pb events is
             categorized by the energy deposited by forward neutrons from
             the struck nucleus. The I_{pPb} values are consistent with
             unity within a few percent for hadrons with
             p_{T}^{ch}>4  GeV at all centralities. These data
             provide new, strong constraints that preclude almost any
             parton energy loss in central p+Pb collisions.},
   Doi = {10.1103/physrevlett.131.072301},
   Key = {fds372604}
}

@booklet{Abachi97,
   Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
             HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard, J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
             MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
             G and Fisk, HE},
   Title = {Studies of gauge boson pair production and trilinear
             couplings},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {56},
   Number = {11},
   Pages = {6742-6778},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.56.6742},
   Abstract = {The gauge boson pair production processes [Formula
             presented], [Formula presented], [Formula presented], and
             [Formula presented] were studied using [Formula presented]
             collisions corresponding to an integrated luminosity of
             approximately [Formula presented] at a center-of-mass energy
             of [Formula presented] TeV. Analysis of [Formula presented]
             production with subsequent [Formula presented] boson decay
             to [Formula presented] [Formula presented] is reported,
             including a fit to the [Formula presented] spectrum of the
             photons which leads to limits on anomalous [Formula
             presented] couplings. A search for [Formula presented]
             production with subsequent decay to [Formula presented]
             [Formula presented] is presented, leading to an upper limit
             on the [Formula presented] production cross section and
             limits on anomalous [Formula presented] and [Formula
             presented] couplings. A search for high [Formula presented]
             [Formula presented] bosons in [Formula presented] and
             [Formula presented] production is described, where one
             [Formula presented] boson decays to an electron and a
             neutrino and the second [Formula presented] boson or the
             [Formula presented] boson decays to two jets. A maximum
             likelihood fit to the [Formula presented] spectrum of
             [Formula presented] bosons resulted in limits on anomalous
             [Formula presented] and [Formula presented] couplings. A
             combined fit to the three data sets which provided the
             tightest limits on anomalous [Formula presented] and
             [Formula presented] couplings is also described. Limits on
             anomalous [Formula presented] and [Formula presented]
             couplings are presented from an analysis of the photon
             [Formula presented] spectrum in [Formula presented] events
             in the decay channels [Formula presented] of the [Formula
             presented] boson. © 1997 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.56.6742},
   Key = {Abachi97}
}

@article{fds345677,
   Author = {Yeh, CH and Chekanov, SV and Kotwal, AV and Proudfoot, J and Sen, S and Tran, NV and Yu, SS},
   Title = {Studies of granularity of a hadronic calorimeter for
             tens-of-TeV jets at a 100 TeV pp collider},
   Journal = {Journal of Instrumentation},
   Volume = {14},
   Number = {5},
   Year = {2019},
   Month = {May},
   url = {http://dx.doi.org/10.1088/1748-0221/14/05/P05008},
   Abstract = {Jet substructure variables for hadronic jets with transverse
             momenta in the range from 2.5 TeV to 20 TeV were studied
             using several designs for the spatial size of calorimeter
             cells. The studies used the full Geant4 simulation of
             calorimeter response combined with realistic reconstruction
             of calorimeter clusters. In most cases, the results indicate
             that the performance of jet-substructure reconstruction
             improves with reducing cell size of a hadronic calorimeter
             from Δ η × Δ φ = 0.087×0.087, which are similar to the
             cell sizes of the calorimeters of LHC experiments, by a
             factor of four, to 0.022×0.022.},
   Doi = {10.1088/1748-0221/14/05/P05008},
   Key = {fds345677}
}

@article{fds310306,
   Author = {Aaltonen, T and Alon, R and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
             A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
             B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
             A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
             F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
             DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
             B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Duchovni, E and Ebina, K and Edgar, R and Elagin,
             A},
   Title = {Studies of high-transverse momentum jet substructure and top
             quarks produced in 1.96 TeV proton-antiproton
             collisions},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {3},
   Year = {2015},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.032006},
   Abstract = {Results of a study of the substructure of the highest
             transverse momentum (pT) jets observed by the CDF
             Collaboration are presented. Events containing at least one
             jet with pT>400GeV/c in a sample corresponding to an
             integrated luminosity of 5.95fb-1, collected in 1.96 TeV
             proton-antiproton collisions at the Fermilab Tevatron
             collider, are selected. A study of the jet mass, angularity,
             and planar-flow distributions is presented, and the
             measurements are compared with predictions of perturbative
             quantum chromodynamics. A search for boosted top-quark
             production is also described, leading to a 95% confidence
             level upper limit of 38 fb on the production cross section
             of top quarks with pT>400GeV/c.},
   Doi = {10.1103/PhysRevD.91.032006},
   Key = {fds310306}
}

@article{fds374252,
   Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
             J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
             W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
             PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
             Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
             MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
             V and Arcangeletti, C and Arce, ATH},
   Title = {Studies of the muon momentum calibration and performance of
             the ATLAS detector with pp collisions at √s=13
             TeV},
   Journal = {European Physical Journal C},
   Volume = {83},
   Number = {8},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-023-11584-x},
   Abstract = {This paper presents the muon momentum calibration and
             performance studies for the ATLAS detector based on the pp
             collisions data sample produced at s = 13 TeV at the LHC
             during Run 2 and corresponding to an integrated luminosity
             of 139 fb - 1 . An innovative approach is used to correct
             for potential charge-dependent momentum biases related to
             the knowledge of the detector geometry, using the Z→
             μ+μ- resonance. The muon momentum scale and resolution are
             measured using samples of J/ ψ→ μ+μ- and Z→ μ+μ-
             events. A calibration procedure is defined and applied to
             simulated data to match the performance measured in real
             data. The calibration is validated using an independent
             sample of Υ → μ+μ- events. At the Z (J/ ψ) peak, the
             momentum scale is measured with an uncertainty at the 0.05%
             (0.1%) level, and the resolution is measured with an
             uncertainty at the 1.5% (2%) level. The charge-dependent
             bias is removed with a dedicated in situ correction for
             momenta up to 450 GeV with a precision better than 0.03 TeV
             - 1 .},
   Doi = {10.1140/epjc/s10052-023-11584-x},
   Key = {fds374252}
}

@article{fds362577,
   Author = {Degrande, C and Holzbauer, JL and Hsu, S-C and Kotwal, AV and Li, S and Marx, M and Mattelaer, O and Metcalfe, J and Pleier, M-A and Pollard, C and Rominsky, M and Wackeroth, D},
   Title = {Studies of Vector Boson Scattering And Triboson Production
             with DELPHES Parametrized Fast Simulation for Snowmass
             2013},
   Year = {2013},
   Month = {September},
   Abstract = {Multiboson production provides a unique way to probe
             Electroweak Symmetry Breaking (EWSB) and physics beyond the
             Standard Model (SM). With the discovery of the Higgs boson,
             the default model is that EWSB occurs according to the Higgs
             mechanism. Deviations from the SM in Higgs and gauge boson
             properties due to new physics at a higher energy scale can
             be parameterized by higher-dimension operators in an
             Effective Field Theory (EFT). We present sensitivity studies
             for dimension-6 and dimension-8 operators in an EFT by
             looking for anomalous vector boson scattering and triboson
             production, at proton-proton colliders with center-of-mass
             energies of 14 TeV, 33 TeV and 100 TeV, respectively.},
   Key = {fds362577}
}

@article{fds212568,
   Author = {A.V. Kotwal and ATLAS Collaboration},
   Title = {Studies of Vector Boson Scattering with an Upgraded ATLAS
             Detector at a High-Luminosity LHC},
   Journal = {ATLAS-PHYS-PUB-2012-005},
   Year = {2012},
   Month = {November},
   Key = {fds212568}
}

@article{fds308219,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon,
             R and Briskin, G and Brock, R and Bross, A and Buchholz, D and Burtovoi,
             VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
             M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
             HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros, Y and Dudko,
             LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
             VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
             OV and Evans, H and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher,
             S and Fein, D and Ferbel, T and Fisk, HE and Fisyak,
             Y},
   Title = {Studies of WW and WZ production and limits on anomalous WWγ
             and WWZ couplings},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {60},
   Number = {7},
   Pages = {1-14},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.60.072002},
   Abstract = {Evidence of anomalous (Formula presented) and (Formula
             presented) production was sought in (Formula presented)
             collisions at a center-of-mass energy of (Formula presented)
             The final states (Formula presented) jet (Formula presented)
             (Formula presented) and (Formula presented) were studied
             using a data sample corresponding to an integrated
             luminosity of approximately (Formula presented) No evidence
             of anomalous diboson production was found. Limits were set
             on anomalous (Formula presented) and (Formula presented)
             couplings and were combined with our previous results. The
             combined 95% confidence level anomalous coupling limits for
             (Formula presented) are (Formula presented) (Formula
             presented) and (Formula presented) (Formula presented)
             assuming the (Formula presented) couplings are equal to the
             (Formula presented) couplings. © 1999 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.60.072002},
   Key = {fds308219}
}

@article{fds356748,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid,
             OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
             J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin,
             T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
             Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Studies of Zγ production in association with a high-mass
             dijet system in pp collisions at √s=8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {7},
   Year = {2017},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2017)107},
   Abstract = {The production of a Z boson and a photon in association with
             a high-mass dijet system is studied using 20.2 fb−1 of
             proton-proton collision data at a centre-of-mass energy of
             s=8 TeV recorded with the ATLAS detector in 2012 at the
             Large Hadron Collider. Final states with a photon and a Z
             boson decaying into a pair of either electrons, muons, or
             neutrinos are analysed. Electroweak and total pp → Zγjj
             cross-sections are extracted in two fiducial regions with
             different sensitivities to electroweak production processes.
             Quartic couplings of vector bosons are studied in regions of
             phase space with an enhanced contribution from pure
             electroweak production, sensitive to vector-boson scattering
             processes VV → Zγ. No deviations from Standard Model
             predictions are observed and constraints are placed on
             anomalous couplings parameterized by higher-dimensional
             operators using effective field theory.[Figure not
             available: see fulltext.].},
   Doi = {10.1007/JHEP07(2017)107},
   Key = {fds356748}
}

@article{fds317299,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
             G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Study of (W/Z)H production and Higgs boson couplings using
             H→ W W decays with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2015)137},
   Abstract = {Abstract: A search for Higgs boson production in association
             with a W or Z boson, in the H→ W W∗ decay channel, is
             performed with a data sample collected with the ATLAS
             detector at the LHC in proton-proton collisions at
             centre-of-mass energies √s=7$$ \sqrt{s}=7 $$ TeV and 8
             TeV, corresponding to integrated luminosities of 4.5 fb−1
             and 20.3 fb−1, respectively. The WH production mode is
             studied in two-lepton and three-lepton final states, while
             two- lepton and four-lepton final states are used to search
             for the ZH production mode. The observed significance, for
             the combined W H and ZH production, is 2.5 standard
             deviations while a significance of 0.9 standard deviations
             is expected in the Standard Model Higgs boson hypothesis.
             The ratio of the combined W H and ZH signal yield to the
             Standard Model expectation, μV H , is found to be μV H =
             3.0− 1.1+ 1.3(stat.)− 0.7+ 1.0(sys.) for the Higgs boson
             mass of 125.36 GeV. The W H and ZH production modes are also
             combined with the gluon fusion and vector boson fusion
             production modes studied in the H → W W∗ → ℓνℓν
             decay channel, resulting in an overall observed significance
             of 6.5 standard deviations and μggF + VBF + VH = 1. 16−
             0.15+ 0.16(stat.)− 0.15+ 0.18(sys.). The results are
             interpreted in terms of scaling factors of the Higgs boson
             couplings to vector bosons (κV ) and fermions (κF ); the
             combined results are: |κV| = 1.06− 0.10+ 0.10, |κF| = 0.
             85− 0.20+ 0.26.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP08(2015)137},
   Key = {fds317299}
}

@article{fds346186,
   Author = {Reddy, D and Kushwaha, AS and Kotwal, A and Basannar, DR and Mahen,
             A},
   Title = {Study of blood pressure profile of school children 6-15
             years in a rural setting of Maharashtra.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {68},
   Number = {3},
   Pages = {222-225},
   Year = {2012},
   Month = {July},
   url = {http://dx.doi.org/10.1016/j.mjafi.2012.03.004},
   Abstract = {<h4>Background</h4>High blood pressure in childhood is a
             major risk factor for heart disease and stroke in adulthood.
             There is enough evidence to suggest that the roots of
             essential hypertension in adults extend into childhood.
             There is a paucity of literature on the blood pressure
             measurements amongst children. This study was done to study
             blood pressure profile of school children in rural area of
             Maharashtra.<h4>Aim & objectives</h4>This cross sectional
             study was carried out to determine the prevalence of
             hypertension in children 6-15 years and to study the
             association between selected variables and blood
             pressure.<h4>Material & methods</h4>This study was done
             using a predesigned questionnaire and making measurements of
             height, BMI and Blood pressure using standardized physical
             instruments following standard guidelines. The data was
             collected and analyzed using appropriate statistical
             tests.<h4>Results</h4>The prevalence of hypertension in the
             study was found to be 4.4% with 3.5% in females and 5.1% in
             males.<h4>Conclusion</h4>In the study, hypertension in
             students was found to be significantly associated with
             higher BMI and with family history of hypertension. Age,
             height and BMI were found to correlate positively with Blood
             pressure levels in this study.},
   Doi = {10.1016/j.mjafi.2012.03.004},
   Key = {fds346186}
}

@article{fds327865,
   Author = {Yu, SS and Chekanov, S and Gray, L and Kotwal, A and Sen, S and Tran,
             NV},
   Title = {Study of boosted W-jets and Higgs-jets with the SiFCC
             detector},
   Journal = {Proceedings of Science},
   Volume = {Part F128556},
   Year = {2016},
   Month = {January},
   Abstract = {We study the detector performance in the reconstruction of
             hadronically-decaying W bosons and Higgs bosons at very high
             energy proton colliders using a full Geant4 simulation of
             the SiFCC detector. The W and Higgs bosons carry transverse
             momentum in the multi-TeV range, which results in collimated
             decay products that are reconstructed as a single jet. We
             present a measurement of the energy response and resolution
             of boosted W-jets and Higgs-jets and show the separation of
             two sub-jets within the boosted boson jet.},
   Key = {fds327865}
}

@article{fds362576,
   Author = {Baak, M and Blondel, A and Bodek, A and Caputo, R and Corbett, T and Degrande, C and Eboli, O and Erler, J and Feigl, B and Freitas, A and Fraile, JG and Gonzalez-Garcia, MC and Haller, J and Han, J and Heinemeyer, S and Hoecker, A and Holzbauer, JL and Hsu, S-C and Jaeger,
             B and Janot, P and Kilian, W and Kogler, R and Kotwal, A and Langacker, P and Li, S and Linssen, L and Marx, M and Mattelaer, O and Metcalfe, J and Monig, K and Moortgat-Pick, G and Pleier, M-A and Pollard, C and Ramsey-Musolf, M and Rauch, M and Reuter, J and Rojo, J and Rominsky, M and Sakumoto, W and Schott, M and Schwinn, C and Sekulla, M and Stelzer, J and Torrence, E and Vicini, A and Wackeroth, D and Weiglein, G and Wilson,
             G and Zeune, L},
   Title = {Study of Electroweak Interactions at the Energy
             Frontier},
   Year = {2013},
   Month = {October},
   Abstract = {With the discovery of the Higgs boson, the spectrum of
             particles in the Standard Model (SM) is complete. It is more
             important than ever to perform precision measurements and to
             test for deviations from SM predictions in the electroweak
             sector. In this report, we investigate two themes in the
             arena of precision electroweak measurements: the electroweak
             precision observables (EWPOs) that test the particle content
             and couplings in the SM and the minimal supersymmetric SM,
             and the measurements involving multiple gauge bosons in the
             final state which provide unique probes of the basic tenets
             of electroweak symmetry breaking. Among the important EWPOs
             we focus our discussion on M_W and sin^2 theta_eff^l, and on
             anomalous quartic gauge couplings probed by triboson
             production and vector boson scattering. We investigate the
             thresholds of precision that need to be achieved in order to
             be sensitive to new physics. We study the precision that can
             be achieved at various facilities on these observables. We
             discuss the calculational tools needed to predict SM rates
             and distributions in order to perform these measurements at
             the required precision. This report summarizes the work of
             the Energy Frontier Precision Study of Electroweak
             Interactions working group of the 2013 Community Summer
             Study (Snowmass).},
   Key = {fds362576}
}

@article{fds321079,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Study of hard double-parton scattering in four-jet events in
             pp collisions at √s=7 TeV with the ATLAS
             experiment},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2016)110},
   Abstract = {Inclusive four-jet events produced in proton-proton
             collisions at a centre-of-mass energy of s=7 TeV are
             analysed for the presence of hard double-parton scattering
             using data corresponding to an integrated luminosity of 37.3
             pb−1, collected with the ATLAS detector at the LHC. The
             contribution of hard double-parton scattering to the
             production of four-jet events is extracted using an
             artificial neural network, assuming that hard double-parton
             scattering can be approximated by an uncorrelated overlaying
             of dijet events. For events containing at least four jets
             with transverse momentum pT ≥ 20 GeV and pseudorapidity
             |η| ≤ 4.4, and at least one having pT ≥ 42.5 GeV, the
             contribution of hard double-parton scattering is estimated
             to be fDPS = 0.092− 0.011+ 0.005(stat.)− 0.037+
             0.033(syst.). After combining this measurement with those of
             the inclusive dijet and four-jet cross-sections in the
             appropriate phase space regions, the effective
             cross-section, σeff , was determined to be σeff = 14. 9−
             1.0+ 1.2(stat.)− 3.8+ 5.1(syst.) mb. This result is
             consistent within the quoted uncertainties with previous
             measurements of σeff , performed at centre-of-mass energies
             between 63 GeV and 8 TeV using various final states, and it
             corresponds to 21− 6+ 7 % of the total inelastic
             cross-section measured at s=7 TeV. The distributions of the
             observables sensitive to the contribution of hard
             double-parton scattering, corrected for detector effects,
             are also provided.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP11(2016)110},
   Key = {fds321079}
}

@article{fds307543,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E and Arik, M and Armbruster, AJ},
   Title = {Study of heavy-flavor quarks produced in association with
             top-quark pairs at s =7TeV using the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.072012},
   Abstract = {Using a sample of dilepton top-quark pair (tt̄) candidate
             events, a study is performed of the production of top-quark
             pairs together with heavy-flavor (HF) quarks, the sum of
             tt̄+b+X and tt̄+c+X, collectively referred to as tt̄+HF.
             The data set used corresponds to an integrated luminosity of
             4.7fb-1 of proton-proton collisions at a center-of-mass
             energy of 7 TeV recorded by the ATLAS detector at the CERN
             Large Hadron Collider. The presence of additional HF (b or
             c) quarks in the tt̄ sample is inferred by looking for
             events with at least three b-tagged jets, where two are
             attributed to the b quarks from the tt̄ decays and the
             third to additional HF production. The dominant background
             to tt̄+HF in this sample is tt̄+jet events in which a
             light-flavor jet is misidentified as a heavy-flavor jet. To
             determine the heavy- and light-flavor content of the
             additional b-tagged jets, a fit to the vertex mass
             distribution of b-tagged jets in the sample is performed.
             The result of the fit shows that 79±14(stat)±22(syst) of
             the 105 selected extra b-tagged jets originate from HF
             quarks, 3 standard deviations away from the hypothesis of
             zero tt̄+HF production. The result for extra HF production
             is quoted as a ratio (RHF) of the cross section for tt̄+HF
             production to the cross section for tt̄ production with at
             least one additional jet. Both cross sections are measured
             in a fiducial kinematic region within the ATLAS acceptance.
             RHF is measured to be [6.2±1.1(stat)±1.8(syst)]% for jets
             with pT>25GeV and |η|<2.5, in agreement with the
             expectations from Monte Carlo generators. © 2014 CERN, for
             the ATLAS Collaboration.},
   Doi = {10.1103/PhysRevD.89.072012},
   Key = {fds307543}
}

@article{fds308152,
   Author = {Acosta, and D, and others},
   Title = {Study of jet shapes in inclusive jet production in p anti-p
             collisions at s**(1/2) = 1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D71},
   Number = {11},
   Pages = {112002},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.112002},
   Abstract = {http://arxiv.org/abs/hep-ex/0505013},
   Doi = {10.1103/PhysRevD.71.112002},
   Key = {fds308152}
}

@article{fds307741,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C},
   Title = {Study of jets produced in association with a W boson in pp
             collisions at √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.092002},
   Abstract = {We report a study of final states containing a W boson and
             hadronic jets, produced in proton-proton collisions at a
             center-of-mass energy of 7 TeV. The data were collected with
             the ATLAS detector at the CERN LHC and comprise the full
             2010 data sample of 36pb-1. Cross sections are determined
             using both the electron and muon decay modes of the W boson
             and are presented as a function of inclusive jet
             multiplicity, Njet, for up to five jets. At each
             multiplicity, cross sections are presented as a function of
             jet transverse momentum, the scalar sum of the transverse
             momenta of the charged lepton, missing transverse momentum,
             and all jets, the invariant mass spectra of jets, and the
             rapidity distributions of various combinations of leptons
             and final-state jets.},
   Doi = {10.1103/PhysRevD.85.092002},
   Key = {fds307741}
}

@article{fds312130,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Study of orbitally excited B mesons and evidence for a new
             Bπ resonance},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {1},
   Pages = {012013},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.012013},
   Abstract = {Using the full CDF Run II data sample, we report evidence
             for a new resonance, which we refer to as B(5970), found
             simultaneously in the B0π+ and B+π- mass distributions
             with a significance of 4.4 standard deviations. We further
             report the first study of resonances consistent with
             orbitally excited B+ mesons and an updated measurement of
             the properties of orbitally excited B0 and Bs0 mesons. We
             measure the masses and widths of all states, as well as the
             relative production rates of the B1, B2*, and B(5970) states
             and the branching fraction of the Bs2*0 state to either
             B*+K- and B+K-. Furthermore, we measure the production rates
             of the orbitally excited B0,+ states relative to the B0,+
             ground state. The masses of the new B(5970) resonances are
             5978±5(stat)±12(syst)MeV/c2 for the neutral state and
             5961±5(stat)±12(syst)MeV/c2 for the charged state,
             assuming that the resonance decays into Bπ final states.
             The properties of the orbitally excited and the new
             B(5970)0,+ states are compatible with isospin symmetry. ©
             2014 American Physical Society.},
   Doi = {10.1103/PhysRevD.90.012013},
   Key = {fds312130}
}

@article{fds356721,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Study of ordered hadron chains with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {96},
   Number = {9},
   Year = {2017},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.96.092008},
   Abstract = {The analysis of the momentum difference between charged
             hadrons in high-energy proton-proton collisions is performed
             in order to study coherent particle production. The observed
             correlation pattern agrees with a model of a helical QCD
             string fragmenting into a chain of ground-state hadrons. A
             threshold momentum difference in the production of adjacent
             pairs of charged hadrons is observed, in agreement with
             model predictions. The presence of low-mass hadron chains
             also explains the emergence of charge-combination-dependent
             two-particle correlations commonly attributed to
             Bose-Einstein interference. The data sample consists of 190
             μb-1 of minimum-bias events collected with proton-proton
             collisions at a center-of-mass energy s=7 TeV in the early
             low-luminosity data taking with the ATLAS detector at the
             LHC.},
   Doi = {10.1103/PhysRevD.96.092008},
   Key = {fds356721}
}

@article{fds307801,
   Author = {Aaltonen, T and Alon, R and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Appel, JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi,
             J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli,
             M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi,
             R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar,
             C and Cuevas, J and Culbertson, R},
   Title = {Study of substructure of high transverse momentum jets
             produced in proton-antiproton collisions at
             √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.091101},
   Abstract = {A study of the substructure of jets with transverse momentum
             greater than 400GeV/c produced in proton-antiproton
             collisions at a center-of-mass energy of 1.96 TeV at the
             Fermilab Tevatron Collider and recorded by the CDF II
             detector is presented. The distributions of the jet mass,
             angularity, and planar flow are measured for the first time
             in a sample with an integrated luminosity of 5.95fb -1. The
             observed substructure for high mass jets is consistent with
             predictions from perturbative quantum chromodynamics. ©
             2012 American Physical Society.},
   Doi = {10.1103/PhysRevD.85.091101},
   Key = {fds307801}
}

@article{fds347522,
   Author = {Aaltonen, T and Albrow, M and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
             A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
             B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
             A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
             F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
             DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
             B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher,
             R},
   Title = {Study of the energy dependence of the underlying event in
             proton-antiproton collisions},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {9},
   Year = {2015},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.092009},
   Abstract = {We study charged particle production (pT>0.5 GeV/c,
             |η|<0.8) in proton-antiproton collisions at total
             center-of-mass energies s=300 GeV, 900 GeV, and 1.96 TeV. We
             use the direction of the charged particle with the largest
             transverse momentum in each event to define three regions of
             η-φ space: "toward", "away", and "transverse." The average
             number and the average scalar pT sum of charged particles in
             the transverse region are sensitive to the modeling of the
             "underlying event." The transverse region is divided into a
             MAX and MIN transverse region, which helps separate the
             "hard component" (initial and final-state radiation) from
             the "beam-beam remnant" and multiple parton interaction
             components of the scattering. The center-of-mass energy
             dependence of the various components of the event is studied
             in detail. The data presented here can be used to constrain
             and improve QCD Monte Carlo models, resulting in more
             precise predictions at the LHC energies of 13 and 14
             TeV.},
   Doi = {10.1103/PhysRevD.92.092009},
   Key = {fds347522}
}

@article{fds356631,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
             S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
             C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S},
   Title = {Study of the hard double-parton scattering contribution to
             inclusive four-lepton production in pp collisions at √s=8
             TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {790},
   Pages = {595-614},
   Year = {2019},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2019.01.062},
   Abstract = {The inclusive production of four isolated charged leptons in
             pp collisions is analysed for the presence of hard
             double-parton scattering, using 20.2 fb−1 of data recorded
             in the ATLAS detector at the LHC at centre-of-mass energy
             s=8 TeV. In the four-lepton invariant-mass range of
             80<m4ℓ<1000 GeV, an artificial neural network is used to
             enhance the separation between single- and double-parton
             scattering based on the kinematics of the four leptons in
             the final state. An upper limit on the fraction of events
             originating from double-parton scattering is determined at
             95% confidence level to be fDPS=0.042, which results in an
             estimated lower limit on the effective cross section at 95%
             confidence level of 1.0 mb.},
   Doi = {10.1016/j.physletb.2019.01.062},
   Key = {fds356631}
}

@article{fds356713,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
             AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
             D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Armitage, LJ},
   Title = {Study of the material of the ATLAS inner detector for Run 2
             of the LHC},
   Journal = {Journal of Instrumentation},
   Volume = {12},
   Number = {12},
   Year = {2017},
   Month = {December},
   url = {http://dx.doi.org/10.1088/1748-0221/12/12/P12009},
   Abstract = {The ATLAS inner detector comprises three different
             sub-detectors: the pixel detector, the silicon strip
             tracker, and the transition-radiation drift-tube tracker.
             The Insertable B-Layer, a new innermost pixel layer, was
             installed during the shutdown period in 2014, together with
             modifications to the layout of the cables and support
             structures of the existing pixel detector. The material in
             the inner detector is studied with several methods, using a
             low-luminosity s=13 TeV pp collision sample corresponding to
             around 2.0 nb-1 collected in 2015 with the ATLAS experiment
             at the LHC. In this paper, the material within the innermost
             barrel region is studied using reconstructed hadronic
             interaction and photon conversion vertices. For the forward
             rapidity region, the material is probed by a measurement of
             the efficiency with which single tracks reconstructed from
             pixel detector hits alone can be extended with hits on the
             track in the strip layers. The results of these studies have
             been taken into account in an improved description of the
             material in the ATLAS inner detector simulation, resulting
             in a reduction in the uncertainties associated with the
             charged-particle reconstruction efficiency determined from
             simulation.},
   Doi = {10.1088/1748-0221/12/12/P12009},
   Key = {fds356713}
}

@article{fds356614,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
             G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
             G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R and Arce, ATH and Ardell, RE and Arduh, FA},
   Title = {Study of the rare decays of B s0 and B
             0 mesons into muon pairs using data collected
             during 2015 and 2016 with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2019},
   Number = {4},
   Year = {2019},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2019)098},
   Abstract = {A study of the decays B s0 → μ + μ − and B 0 → μ +
             μ − has been performed using 26.3 fb −1 of 13 TeV LHC
             proton-proton collision data collected with the ATLAS
             detector in 2015 and 2016. Since the detector resolution in
             μ + μ − invariant mass is comparable to the B s0 -B 0
             mass difference, a single fit determines the signal yields
             for both decay modes. This results in a measurement of the
             branching fraction ℬ(Bs0→μ+μ−)=(3.2−1.0+1.1)×10−9
             and an upper limit ℬ (B→ μ + μ − ) < 4.3 × 10 −
             10 at 95% confidence level. The result is combined with the
             Run 1 ATLAS result, yielding ℬ(Bs0→μ+μ−)=(2.8−0.7+0.8)×10−9
             and ℬ (B→ μ + μ − ) < 2.1 × 10 − 10 at 95%
             confidence level. The combined result is consistent with the
             Standard Model prediction within 2.4 standard deviations in
             the ℬ(B0→μ+μ−)−ℬ(Bs0→μ+μ−) plane.[Figure
             not available: see fulltext.]},
   Doi = {10.1007/JHEP04(2019)098},
   Key = {fds356614}
}

@article{fds321094,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
             N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
             F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
             EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
             R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán,
             SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura,
             P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana,
             S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
             A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A},
   Title = {Study of the rare decays of [Formula: see text] and
             [Formula: see text] into muon pairs from data collected
             during the LHC Run 1 with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {9},
   Pages = {513},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4338-8},
   Abstract = {A study of the decays [Formula: see text] and [Formula: see
             text] has been performed using data corresponding to an
             integrated luminosity of 25 fb[Formula: see text] of 7 and
             8 TeV proton-proton collisions collected with the ATLAS
             detector during the LHC Run 1. For the [Formula: see text]
             dimuon decay, an upper limit on the branching fraction is
             set at [Formula: see text] at 95 % confidence level. For
             [Formula: see text], the branching fraction [Formula: see
             text] is measured. The results are consistent with the
             Standard Model expectation with a <i>p</i> value of 4.8 %,
             corresponding to 2.0 standard deviations.},
   Doi = {10.1140/epjc/s10052-016-4338-8},
   Key = {fds321094}
}

@article{fds346166,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
             C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
             MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
             N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black,
             CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet,
             D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero,
             J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
             S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chiodini,
             G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
             K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot,
             J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis,
             E},
   Title = {Study of the spin and parity of the Higgs boson in diboson
             decays with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {10},
   Pages = {476},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3685-1},
   Abstract = {Studies of the spin, parity and tensor couplings of the
             Higgs boson in the [Formula: see text], [Formula: see text]
             and [Formula: see text] decay processes at the LHC are
             presented. The investigations are based on [Formula: see
             text] of <i>pp</i> collision data collected by the ATLAS
             experiment at [Formula: see text] TeV and [Formula: see
             text] TeV. The Standard Model (SM) Higgs boson hypothesis,
             corresponding to the quantum numbers [Formula: see text], is
             tested against several alternative spin scenarios, including
             non-SM spin-0 and spin-2 models with universal and
             non-universal couplings to fermions and vector bosons. All
             tested alternative models are excluded in favour of the SM
             Higgs boson hypothesis at more than 99.9 % confidence
             level. Using the [Formula: see text] and [Formula: see text]
             decays, the tensor structure of the interaction between the
             spin-0 boson and the SM vector bosons is also investigated.
             The observed distributions of variables sensitive to the
             non-SM tensor couplings are compatible with the SM
             predictions and constraints on the non-SM couplings are
             derived.},
   Doi = {10.1140/epjc/s10052-015-3685-1},
   Key = {fds346166}
}

@booklet{Abachi97e,
   Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
             HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard, J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
             MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
             G and Fisk, HE},
   Title = {Study of the ZZγ and Zγγ Couplings
             in Z(νν)γ Production},
   Journal = {Physical Review Letters},
   Volume = {78},
   Number = {19},
   Pages = {3640-3645},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.78.3640},
   Abstract = {We have measured the ZZγ and ZZγ couplings by studying
             13.1 pb−1 of pp¯→Etγ+ X data at √s = 1.8 TeV with
             the Dø detector at the Fermilab Tevatron Collider. This is
             the first study of hadronic Zγ production in the neutrino
             decay channel. Combining this measurement with our previous
             results using Z→ee and μμ yields the most stringent 95%
             C.L. limits to date on anomalous couplings: |h30Z|<0.4,
             |h40Z|<0.06 (λ=750 GeV. © 1997 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.78.3640},
   Key = {Abachi97e}
}

@article{fds346164,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly,
             IA},
   Title = {Study of the [Formula: see text] and [Formula: see text]
             decays with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {4},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3743-8},
   Abstract = {The decays [Formula: see text] and [Formula: see text] are
             studied with the ATLAS detector at the LHC using a dataset
             corresponding to integrated luminosities of 4.9 and 20.6
             fb[Formula: see text] of <i>pp</i> collisions collected at
             centre-of-mass energies [Formula: see text] TeV and 8 TeV,
             respectively. Signal candidates are identified through
             [Formula: see text] and [Formula: see text] decays. With a
             two-dimensional likelihood fit involving the [Formula: see
             text] reconstructed invariant mass and an angle between the
             [Formula: see text] and [Formula: see text] candidate
             momenta in the muon pair rest frame, the yields of [Formula:
             see text] and [Formula: see text], and the transverse
             polarisation fraction in [Formula: see text] decay are
             measured. The transverse polarisation fraction is determined
             to be [Formula: see text], and the derived ratio of the
             branching fractions of the two modes is [Formula: see text],
             where the first error is statistical and the second is
             systematic. Finally, a sample of [Formula: see text] decays
             is used to derive the ratios of branching fractions
             [Formula: see text] and [Formula: see text], where the third
             error corresponds to the uncertainty of the branching
             fraction of [Formula: see text] decay. The available
             theoretical predictions are generally consistent with the
             measurement.},
   Doi = {10.1140/epjc/s10052-015-3743-8},
   Key = {fds346164}
}

@article{fds307535,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Study of top quark production and decays involving a tau
             lepton at CDF and limits on a charged Higgs boson
             contribution},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.091101},
   Abstract = {We present an analysis of top-antitop quark production and
             decay into a tau lepton, tau neutrino, and bottom quark
             using data from 9fb-1 of integrated luminosity at the
             Collider Detector at Fermilab. Dilepton events, where one
             lepton is an energetic electron or muon and the other a
             hadronically decaying tau lepton, originating from
             proton-antiproton collisions at s=1.96TeV, are used. A
             top-antitop quark production cross section of 8.1±2.1pb is
             measured, assuming standard-model top quark decays. By
             separately identifying for the first time the single-tau and
             the ditau components, we measure the branching fraction of
             the top quark into the tau lepton, tau neutrino, and bottom
             quark to be (9.6±2.8)%. The branching fraction of top quark
             decays into a charged Higgs boson and a bottom quark, which
             would imply violation of lepton universality, is limited to
             be less than 5.9% at a 95% confidence level [for
             B(H-→τν̄)=1]. © 2014 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.89.091101},
   Key = {fds307535}
}

@article{fds348984,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov,
             VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel,
             M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
             A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz,
             T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black,
             KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
             SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
             B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
             E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Gimenez, VC and Castro,
             NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
             YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
             YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C},
   Title = {Study of W W γ and W Z γ production in p p collisions at s
             = 8 TeV and search for anomalous quartic gauge couplings
             with the ATLAS experiment.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {9},
   Pages = {646},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5180-3},
   Abstract = {This paper presents a study of W W γ and W Z γ triboson
             production using events from proton-proton collisions at a
             centre-of-mass energy of s = 8 TeV recorded with the ATLAS
             detector at the LHC and corresponding to an integrated
             luminosity of 20.2 fb - 1 . The W W γ production
             cross-section is determined using a final state containing
             an electron, a muon, a photon, and neutrinos ( e ν μ ν γ
             ). Upper limits on the production cross-section of the e ν
             μ ν γ final state and the W W γ and W Z γ final states
             containing an electron or a muon, two jets, a photon, and a
             neutrino ( e ν j j γ or μ ν j j γ ) are also derived.
             The results are compared to the cross-sections predicted by
             the Standard Model at next-to-leading order in the
             strong-coupling constant. In addition, upper limits on the
             production cross-sections are derived in a fiducial region
             optimised for a search for new physics beyond the Standard
             Model. The results are interpreted in the context of
             anomalous quartic gauge couplings using an effective field
             theory. Confidence intervals at 95% confidence level are
             derived for the 14 coupling coefficients to which W W γ and
             W Z γ production are sensitive.},
   Doi = {10.1140/epjc/s10052-017-5180-3},
   Key = {fds348984}
}

@article{fds307924,
   Author = {Aaltonen, and T, and others},
   Title = {Studying the Underlying Event in Drell-Yan and High
             Transverse Momentum Jet Production at the
             Tevatron},
   Journal = {Phys. Rev.},
   Volume = {D82},
   Number = {3},
   Pages = {034001},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.034001},
   Abstract = {http://arxiv.org/abs/1003.3146},
   Doi = {10.1103/PhysRevD.82.034001},
   Key = {fds307924}
}

@article{fds331390,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon,
             TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
             VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
             F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and De Jong and SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros,
             Y},
   Title = {Subjet multiplicity of gluon and quark jets reconstructed
             with the κ algorithm in pp̄
             collisions},
   Journal = {Physical Review D},
   Volume = {65},
   Number = {5},
   Pages = {20},
   Publisher = {American Physical Society (APS)},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.65.052008},
   Abstract = {The DØ Collaboration has studied for the first time the
             properties of hadron-collider jets reconstructed with a
             successive-combination algorithm based on relative
             transverse momenta (κ⊥) of energy clusters. Using the
             standard value D = 1.0 of the jet-separation parameter in
             the κ⊥ algorithm, we find that the pT of such jets is
             higher than the ET of matched jets reconstructed with cones
             of radius R = 0.7, by about 5 (8) GeV at pT ≈90 (240) GeV.
             To examine internal jet structure, the κ⊥ algorithm is
             applied within D = 0.5 jets to resolve any subjets. The
             multiplicity of subjets in jet samples at √s = 1800 GeV
             and 630 GeV is extracted separately for gluons (Mg) and
             quarks (Mq), and the ratio of average subjet multiplicities
             in gluon and quark jets is measured as (〈Mg〉-1)/(〈Mq〉-1)
             = 1.84±0.15 (stat)±0.180.22 (syst). This ratio is in
             agreement with the expectations from the HERWIG Monte Carlo
             event generator and a resummation calculation, and with
             observations in e+e- annihilations, and is close to the
             naive prediction for the ratio of color charges of CA /CF =
             9/4 = 2.25.},
   Doi = {10.1103/PhysRevD.65.052008},
   Key = {fds331390}
}

@article{fds347527,
   Author = {Dwivedi, DA and Alasinga, S and Singhal, S and Malhotra, VK and Kotwal,
             A},
   Title = {Successful treatment of frostbite with hyperbaric oxygen
             treatment.},
   Journal = {Indian journal of occupational and environmental
             medicine},
   Volume = {19},
   Number = {2},
   Pages = {121-122},
   Year = {2015},
   Month = {May},
   url = {http://dx.doi.org/10.4103/0019-5278.165336},
   Doi = {10.4103/0019-5278.165336},
   Key = {fds347527}
}

@article{fds313609,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Summary of the ATLAS experiment’s sensitivity to
             supersymmetry after LHC Run 1 — interpreted in the
             phenomenological MSSM},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2015)134},
   Abstract = {Abstract: A summary of the constraints from the ATLAS
             experiment on R-parity-conserving supersymmetry is
             presented. Results from 22 separate ATLAS searches are
             considered, each based on analysis of up to 20.3 fb−1 of
             proton-proton collision data at centre-of-mass energies of
             s=7$$ \sqrt{s}=7 $$ and 8 TeV at the Large Hadron Collider.
             The results are interpreted in the context of the
             19-parameter phenomenological minimal supersymmetric
             standard model, in which the lightest supersymmetric
             particle is a neutralino, taking into account constraints
             from previous precision electroweak and flavour measurements
             as well as from dark matter related measurements. The
             results are presented in terms of constraints on
             supersymmetric particle masses and are compared to limits
             from simplified models. The impact of ATLAS searches on
             parameters such as the dark matter relic density, the
             couplings of the observed Higgs boson, and the degree of
             electroweak fine-tuning is also shown. Spectra for surviving
             supersymmetry model points with low fine-tunings are
             presented.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP10(2015)134},
   Key = {fds313609}
}

@article{fds313604,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Summary of the searches for squarks and gluinos using √s =
             8 TeV pp collisions with the ATLAS experiment at the
             LHC},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2015)054},
   Abstract = {Abstract: A summary is presented of ATLAS searches for
             gluinos and first- and second-generation squarks in final
             states containing jets and missing transverse momentum, with
             or without leptons or b-jets, in the s=8$$ \sqrt{s}=8 $$ TeV
             data set collected at the Large Hadron Collider in 2012.
             This paper reports the results of new interpretations and
             statistical combinations of previously published analyses,
             as well as a new analysis. Since no significant excess of
             events over the Standard Model expectation is observed, the
             data are used to set limits in a variety of models. In all
             the considered simplified models that assume R-parity
             conservation, the limit on the gluino mass exceeds 1150 GeV
             at 95% confidence level, for an LSP mass smaller than 100
             GeV. Furthermore, exclusion limits are set for left-handed
             squarks in a phenomenological MSSM model, a minimal
             Supergravity/Constrained MSSM model, R-parity-violation
             scenarios, a minimal gauge-mediated supersymmetry breaking
             model, a natural gauge mediation model, a non-universal
             Higgs mass model with gaugino mediation and a minimal model
             of universal extra dimensions.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP10(2015)054},
   Key = {fds313604}
}

@article{fds372387,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam
             Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
             F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
             Camelia, E and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral
             Coutinho, Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
             SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
             AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
             M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo,
             JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol,
             AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari,
             T and Barisits, M-S and Barklow, T and Barnett, RM and Baron, P and Baron
             Moreno, DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco
             Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
             M and Battulga, D and Bauce, M and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos,
             P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun,
             D and Bendebba, F and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram,
             IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biglietti, M and Billoud,
             TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Bisceglie,
             E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
             JE and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Britton, D and Britzger, D and Brock,
             I and Brooijmans, G and Brooks, WK and Brost, E and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
             EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
             AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
             Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson,
             BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter,
             JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
             DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chiu, YH and Chizhov,
             MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
             BM and Clark, A and Clark, PJ and Clavijo Columbie,
             JM},
   Title = {Test of CP Invariance in Higgs Boson Vector-Boson-Fusion
             Production Using the H→γγ Channel with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {131},
   Number = {6},
   Pages = {061802},
   Year = {2023},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.131.061802},
   Abstract = {A test of CP invariance in Higgs boson production via
             vector-boson fusion has been performed in the H→γγ
             channel using 139  fb^{-1} of proton-proton collision
             data at sqrt[s]=13  TeV collected by the ATLAS detector
             at the LHC. The optimal observable method is used to probe
             the CP structure of interactions between the Higgs boson and
             electroweak gauge bosons, as described by an effective field
             theory. No sign of CP violation is observed in the data.
             Constraints are set on the parameters describing the
             strength of the CP-odd component in the coupling between the
             Higgs boson and the electroweak gauge bosons in two
             effective field theory bases: d[over ˜] in the HISZ basis
             and c_{HW[over ˜]} in the Warsaw basis. The results
             presented are the most stringent constraints on CP violation
             in the coupling between Higgs and weak bosons. The 95% C.L.
             constraint on d[over ˜] is derived for the first time and
             the 95% C.L. constraint on c_{HW[over ˜]} has been improved
             by a factor of 5 compared to the previous
             measurement.},
   Doi = {10.1103/physrevlett.131.061802},
   Key = {fds372387}
}

@article{fds349776,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH},
   Title = {Test of CP invariance in vector-boson fusion production of
             the Higgs boson in the H → ττ channel in
             proton–proton collisions at [Formula presented] with the
             ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {805},
   Year = {2020},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.physletb.2020.135426},
   Abstract = {A test of CP invariance in Higgs boson production via
             vector-boson fusion is performed in the H→ττ decay
             channel. This test uses the Optimal Observable method and is
             carried out using 36.1fb−1 of s=13TeV proton–proton
             collision data collected by the ATLAS experiment at the LHC.
             Contributions from CP-violating interactions between the
             Higgs boson and electroweak gauge bosons are described by an
             effective field theory, in which the parameter d˜ governs
             the strength of CP violation. No sign of CP violation is
             observed in the distributions of the Optimal Observable, and
             d˜ is constrained to the interval [−0.090, 0.035] at the
             68% confidence level (CL), compared to an expected interval
             of d˜∈[−0.035,0.033] based upon the Standard Model
             prediction. No constraints can be set on d˜ at 95% CL,
             while an expected 95% CL interval of d˜∈[−0.21,0.15]
             for the Standard Model hypothesis was expected.},
   Doi = {10.1016/j.physletb.2020.135426},
   Key = {fds349776}
}

@article{fds322002,
   Author = {Aad, G and Abbott, B and Abdinov, O and Abdallah, J and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako,
             K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro,
             LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund,
             OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan,
             AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel,
             O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
             T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
             E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito,
             L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas,
             CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou,
             Y},
   Title = {Test of CP invariance in vector-boson fusion production of
             the Higgs boson using the Optimal Observable method
             in the ditau decay channel with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {12},
   Pages = {658},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4499-5},
   Abstract = {A test of CP invariance in Higgs boson production via
             vector-boson fusion using the method of the <i>Optimal
             Observable</i> is presented. The analysis exploits the decay
             mode of the Higgs boson into a pair of [Formula: see text]
             leptons and is based on 20.3 [Formula: see text] of
             proton-proton collision data at [Formula: see text] =
             8 [Formula: see text] collected by the ATLAS experiment at
             the LHC. Contributions from CP-violating interactions
             between the Higgs boson and electroweak gauge bosons are
             described in an effective field theory framework, in which
             the strength of CP violation is governed by a single
             parameter [Formula: see text]. The mean values and
             distributions of CP-odd observables agree with the
             expectation in the Standard Model and show no sign of CP
             violation. The CP-mixing parameter [Formula: see text] is
             constrained to the interval [Formula: see text] at 68%
             confidence level, consistent with the Standard Model
             expectation of [Formula: see text].},
   Doi = {10.1140/epjc/s10052-016-4499-5},
   Key = {fds322002}
}

@article{fds357656,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
             A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
             K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
             M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
             EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso,
             S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen,
             T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
             CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
             DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
   Title = {Test of the universality of τ and μ lepton couplings in
             W-boson decays with the ATLAS detector},
   Journal = {Nature Physics},
   Volume = {17},
   Number = {7},
   Pages = {813-818},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2021},
   Month = {July},
   url = {http://dx.doi.org/10.1038/s41567-021-01236-w},
   Abstract = {The standard model of particle physics encapsulates our best
             current understanding of physics at the smallest scales. A
             fundamental axiom of this theory is the universality of the
             couplings of the different generations of leptons to the
             electroweak gauge bosons. The measurement of the ratio of
             the decay rate of W bosons to τ leptons and muons,
             R(τ/μ), constitutes an important test of this axiom. Using
             139 fb−1 of proton–proton collisions recorded with the
             ATLAS detector at a centre-of-mass energy of 13 TeV, we
             report a measurement of this quantity from di-leptonic tt¯
             events where the top quarks decay into a W boson and a
             bottom quark. We can distinguish muons originating from W
             bosons and those originating from an intermediate τ lepton
             through the muon transverse impact parameter and differences
             in the muon transverse momentum spectra. The measured value
             of R(τ/μ) is 0.992 ± 0.013 [± 0.007(stat) ±
             0.011(syst)] and is in agreement with the hypothesis of
             universal lepton couplings as postulated in the standard
             model. This is the only such measurement from the Large
             Hadron Collider, so far, and obtains twice the precision of
             previous measurements.},
   Doi = {10.1038/s41567-021-01236-w},
   Key = {fds357656}
}

@article{fds313603,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
             T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
             R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
             D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt,
             O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown,
             D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu, A and Calamba, A and Camacho-Pérez, E and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chakrabarti, S and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Cihangir, S and Claes, D and Clark, A and Clarke, C and Clutter, J and Convery, ME and Conway, J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox,
             CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson,
             R and Cutts, D and Das, A and d'Ascenzo, N and Datta, M and Davies, G and de
             Barbaro, P and de Jong, SJ and De La Cruz-Burelo and E and Déliot, F and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov,
             SP and D'Errico, M and Desai, S and Deterre, C and DeVaughan, K and Devoto,
             F and Di Canto and A and Di Ruzza and B and Diehl, HT and Diesburg, M and Ding,
             PF and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Dubey, A and Dudko, LV and Duperrin, A and Dutt, S and Eads, M and Ebina, K and Edgar, R and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Erbacher, R and Errede, S and Esham, B and Evans, H and Evdokimov, A and Evdokimov, VN and Farrington,
             S and Fauré, A and Feng, L and Ferbel, T and Fernández Ramos and JP and Fiedler, F and Field, R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest, R and Fortner, M and Fox, H and Franklin, M and Freeman, JC and Frisch, H and Fuess, S and Funakoshi, Y and Galloni, C and Garbincius, PH and Garcia-Bellido, A and García-González, JA and Garfinkel, AF and Garosi, P and Gavrilov, V and Geng, W and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gogota, O and Gold, M and Goldin, D and Golossanov, A and Golovanov, G and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López,
             O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grannis, PD and Greder, S and Greenlee, H and Grenier, G and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald, MW and Guillemin, T and Guimaraes da
             Costa, J and Gutierrez, G and Gutierrez, P and Hahn, SR and Haley, J and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, M and Harel, A and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hauptman, JM and Hays, C and Hays, J and Head, T and Hebbeker, T and Hedin,
             D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hildreth, MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen, B and Hogan, J and Hohlfeld, M and Holzbauer, JL and Hong, Z and Hopkins, W and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeon, EJ and Jeong, MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere, A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun,
             SY and Jung, AW and Junk, TR and Juste, A and Kajfasz, E and Kambeitz, M and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kato, Y and Katsanos, I and Kaur, M and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava, A and Kharzheev, YN and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Kiselevich, I and Knoepfel, K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Laasanen, AT and Lammel, S and Lammers, S and Lancaster, M and Lannon, K and Latino, G and Lebrun, P and Lee, HS and Lee, JS and Lee, SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis, JD and Li, D and Li, H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Liu, H and Liu, Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lys, J and Lysak, R and Maciel, AKA and Madar, R and Madrak, R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G and Manousakis-Katsikakis, A and Mansour, J and Marchese, L and Margaroli, F and Marino, P and Martínez-Ortega, J and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McCarthy, R and McGivern, CL and McNulty, R and Mehta, A and Mehtala, P and Meijer, MM and Melnitchouk, A and Menezes, D and Mercadante, PG and Merkin, M and Mesropian, C and Meyer, A and Meyer, J and Miao, T and Miconi, F and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondal, NK and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Mulhearn, M and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nagy, E and Nakano, I and Napier, A and Narain, M and Nayyar, R and Neal, HA and Negret, JP and Nett, J and Neu, C and Neustroev, P},
   Title = {Tevatron Combination of Single-Top-Quark Cross Sections and
             Determination of the Magnitude of the Cabibbo-Kobayashi-Maskawa
             Matrix Element V_{tb}.},
   Journal = {Physical review letters},
   Volume = {115},
   Number = {15},
   Pages = {152003},
   Year = {2015},
   Month = {October},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.115.152003},
   Abstract = {We present the final combination of CDF and D0 measurements
             of cross sections for single-top-quark production in
             proton-antiproton collisions at a center-of-mass energy of
             1.96 TeV. The data correspond to total integrated
             luminosities of up to 9.7 fb^{-1} per experiment. The
             t-channel cross section is measured to be
             σ_{t}=2.25_{-0.31}^{+0.29} pb. We also present the
             combinations of the two-dimensional measurements of the s-
             vs t-channel cross section. In addition, we give the
             combination of the s+t channel cross section measurement
             resulting in σ_{s+t}=3.30_{-0.40}^{+0.52} pb, without
             assuming the standard model value for the ratio
             σ_{s}/σ_{t}. The resulting value of the magnitude of the
             top-to-bottom quark coupling is |V_{tb}|=1.02_{-0.05}^{+0.06},
             corresponding to |V_{tb}|>0.92 at the 95%
             C.L.},
   Doi = {10.1103/physrevlett.115.152003},
   Key = {fds313603}
}

@article{fds310289,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
             T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
             R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
             D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt,
             O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown,
             D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu, A and Calamba, A and Camacho-Pérez, E and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chakrabarti, S and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Cihangir, S and Claes, D and Clark, A and Clarke, C and Clutter, J and Convery, ME and Conway, J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox,
             CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson,
             R and Cutts, D and Das, A and d'Ascenzo, N and Datta, M and Davies, G and de
             Barbaro, P and de Jong, SJ and De La Cruz-Burelo and E and Déliot, F and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov,
             SP and D'Errico, M and Desai, S and Deterre, C and DeVaughan, K and Devoto,
             F and Di Canto and A and Di Ruzza and B and Diehl, HT and Diesburg, M and Ding,
             PF and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Dubey, A and Dudko, LV and Duperrin, A and Dutt, S and Eads, M and Ebina, K and Edgar, R and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Erbacher, R and Errede, S and Esham, B and Evans, H and Evdokimov, VN and Farrington, S and Fauré, A and Feng, L and Ferbel, T and Fernández Ramos and JP and Fiedler, F and Field,
             R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest,
             R and Fortner, M and Fox, H and Franklin, M and Freeman, JC and Frisch, H and Fuess, S and Funakoshi, Y and Galloni, C and Garbincius, PH and Garcia-Bellido, A and García-González, JA and Garfinkel, AF and Garosi, P and Gavrilov, V and Geng, W and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini,
             P and Glagolev, V and Glenzinski, D and Gogota, O and Gold, M and Goldin,
             D and Golossanov, A and Golovanov, G and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grannis, PD and Greder, S and Greenlee, H and Grenier, G and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald,
             MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hahn, SR and Haley, J and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, M and Harel, A and Harr,
             RF and Harrington-Taber, T and Hatakeyama, K and Hauptman, JM and Hays,
             C and Hays, J and Head, T and Hebbeker, T and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De
             La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hildreth, MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen, B and Hogan, J and Hohlfeld, M and Holzbauer, JL and Hong, Z and Hopkins, W and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeon, EJ and Jeong, MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere,
             A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung,
             AW and Junk, TR and Juste, A and Kajfasz, E and Kambeitz, M and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kato, Y and Katsanos, I and Kaur, M and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava, A and Kharzheev, YN and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Kiselevich,
             I and Knoepfel, K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg,
             J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Laasanen, AT and Lammel, S and Lammers, S and Lancaster,
             M and Lannon, K and Latino, G and Lebrun, P and Lee, HS and Lee, JS and Lee,
             SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis,
             JD and Li, D and Li, H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Liu, H and Liu, Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lys, J and Lysak, R and Maciel, AKA and Madar, R and Madrak, R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G and Manousakis-Katsikakis, A and Mansour, J and Marchese, L and Margaroli, F and Marino, P and Martínez-Ortega, J and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McCarthy, R and McGivern, CL and McNulty, R and Mehta, A and Mehtala, P and Meijer, MM and Melnitchouk, A and Menezes, D and Mercadante, PG and Merkin, M and Mesropian, C and Meyer, A and Meyer, J and Miao, T and Miconi, F and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondal, NK and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Mulhearn, M and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nagy, E and Nakano, I and Napier, A and Narain, M and Nayyar, R and Neal, HA and Negret, JP and Nett, J and Neu, C and Neustroev, P and Nguyen, HT},
   Title = {Tevatron constraints on models of the Higgs boson with
             exotic spin and parity using decays to bottom-antibottom
             quark pairs.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {15},
   Pages = {151802},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.114.151802},
   Abstract = {Combined constraints from the CDF and D0 Collaborations on
             models of the Higgs boson with exotic spin J and parity P
             are presented and compared with results obtained assuming
             the standard model value JP=0+. Both collaborations analyzed
             approximately 10  fb(-) of proton-antiproton collisions
             with a center-of-mass energy of 1.96 TeV collected at the
             Fermilab Tevatron. Two models predicting exotic Higgs bosons
             with JP=0- and JP=2+ are tested. The kinematic properties of
             exotic Higgs boson production in association with a vector
             boson differ from those predicted for the standard model
             Higgs boson. Upper limits at the 95% credibility level on
             the production rates of the exotic Higgs bosons, expressed
             as fractions of the standard model Higgs boson production
             rate, are set at 0.36 for both the JP=0- hypothesis and the
             JP=2+ hypothesis. If the production rate times the branching
             ratio to a bottom-antibottom pair is the same as that
             predicted for the standard model Higgs boson, then the
             exotic bosons are excluded with significances of 5.0
             standard deviations and 4.9 standard deviations for the
             JP=0- and JP=2+ hypotheses, respectively.},
   Doi = {10.1103/physrevlett.114.151802},
   Key = {fds310289}
}

@article{fds356677,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Aushev, V and Aushev, Y and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
             JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
             SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brochmann,
             M and Brock, R and Bromberg, C and Bross, A and Brown, D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto,
             G},
   Title = {Tevatron Run II combination of the effective leptonic
             electroweak mixing angle},
   Journal = {Physical Review D},
   Volume = {97},
   Number = {11},
   Year = {2018},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.97.112007},
   Abstract = {Drell-Yan lepton pairs produced in the process
             pp→â.,"+â.,"-+X through an intermediate γ∗/Z boson
             have an asymmetry in their angular distribution related to
             the spontaneous symmetry breaking of the electroweak force
             and the associated mixing of its neutral gauge bosons. The
             CDF and D0 experiments have measured the effective-leptonic
             electroweak mixing parameter sin2θefflept using electron
             and muon pairs selected from the full Tevatron
             proton-antiproton data sets collected in 2001-2011,
             corresponding to 9-10 fb-1 of integrated luminosity. The
             combination of these measurements yields the most precise
             result from hadron colliders, sin2θefflept=0.23148±0.00033.
             This result is consistent with, and approaches in precision,
             the best measurements from electron-positron colliders. The
             standard model inference of the on-shell electroweak mixing
             parameter sin2θW, or equivalently the W-boson mass MW,
             using the zfitter software package yields
             sin2θW=0.22324±0.00033 or equivalently, MW=80.367±0.017
             GeV/c2.},
   Doi = {10.1103/PhysRevD.97.112007},
   Key = {fds356677}
}

@article{fds359004,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
             J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
             G and Alison, J and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
             MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
             JK and Anderson, JT and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira,
             RA},
   Title = {The ATLAS fast TracKer system},
   Journal = {Journal of Instrumentation},
   Volume = {16},
   Number = {7},
   Year = {2021},
   Month = {July},
   url = {http://dx.doi.org/10.1088/1748-0221/16/07/P07006},
   Abstract = {The ATLAS Fast TracKer (FTK) was designed to provide full
             tracking for the ATLAS high-level trigger by using pattern
             recognition based on Associative Memory (AM) chips and
             fitting in high-speed field programmable gate arrays. The
             tracks found by the FTK are based on inputs from all modules
             of the pixel and silicon microstrip trackers. The as-built
             FTK system and components are described, as is the online
             software used to control them while running in the ATLAS
             data acquisition system. Also described is the simulation of
             the FTK hardware and the optimization of the AM pattern
             banks. An optimization for long-lived particles with large
             impact parameter values is included. A test of the FTK
             system with the data playback facility that allowed the FTK
             to be commissioned during the shutdown between Run 2 and Run
             3 of the LHC is reported. The resulting tracks from part of
             the FTK system covering a limited η-ϕ region of the
             detector are compared with the output from the FTK
             simulation. It is shown that FTK performance is in good
             agreement with the simulation.},
   Doi = {10.1088/1748-0221/16/07/P07006},
   Key = {fds359004}
}

@article{fds362780,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
             J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
             X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
             M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C and Arce, ATH and Arguin, JF},
   Title = {The ATLAS inner detector trigger performance in pp
             collisions at 13 TeV during LHC Run 2},
   Journal = {European Physical Journal C},
   Volume = {82},
   Number = {3},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2022},
   Month = {March},
   url = {http://dx.doi.org/10.1140/epjc/s10052-021-09920-0},
   Abstract = {The design and performance of the inner detector trigger for
             the high level trigger of the ATLAS experiment at the Large
             Hadron Collider during the 2016–2018 data taking period is
             discussed. In 2016, 2017, and 2018 the ATLAS detector
             recorded 35.6fb-1, 46.9fb-1, and 60.6fb-1 respectively of
             proton–proton collision data at a centre-of-mass energy of
             13 TeV. In order to deal with the very high interaction
             multiplicities per bunch crossing expected with the 13 TeV
             collisions the inner detector trigger was redesigned during
             the long shutdown of the Large Hadron Collider from 2013
             until 2015. An overview of these developments is provided
             and the performance of the tracking in the trigger for the
             muon, electron, tau and b-jet signatures is discussed. The
             high performance of the inner detector trigger with these
             extreme interaction multiplicities demonstrates how the
             inner detector tracking continues to lie at the heart of the
             trigger performance and is essential in enabling the ATLAS
             physics programme.},
   Doi = {10.1140/epjc/s10052-021-09920-0},
   Key = {fds362780}
}

@article{fds308205,
   Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bean, A and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar,
             V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
             G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler,
             M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
             D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl,
             OI and Davis, K and De, K and del Signore, K and Demarteau, M and Denisov,
             D and Denisov, SP and Diehl, HT and Diesburg, M and di Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann,
             R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein,
             D},
   Title = {The bb̄ production cross section and angular correlations
             in pp̄ collisions at √s = 1.8 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {487},
   Number = {3-4},
   Pages = {264-272},
   Publisher = {Elsevier BV},
   Year = {2000},
   Month = {August},
   url = {http://dx.doi.org/10.1016/S0370-2693(00)00844-3},
   Abstract = {We present measurements of the bb̄ production cross section
             and angular correlations using the DO detector at the
             Fermilab Tevatron pp̄ Collider operating at √s = 1.8 TeV.
             The b quark production cross section for |y(b)| < 1.0 and
             p(T)/b > 6 GeV/c is extracted from single muon and dimuon
             data samples. The results agree in shape with the
             next-to-leading order QCD calculation of heavy flavor
             production but are greater than the central values of these
             predictions. The angular correlations between b and b̄
             quarks, measured from the azimuthal opening angle between
             their decay muons, also agree in shape with the
             next-to-leading order QCD prediction. (C) 2000 Elsevier
             Science B.V.},
   Doi = {10.1016/S0370-2693(00)00844-3},
   Key = {fds308205}
}

@article{fds310385,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
             T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt,
             J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
             R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez
             Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
             A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M},
   Title = {The differential production cross section of the [Formula:
             see text](1020) meson in [Formula: see text] = 7 TeV
             [Formula: see text] collisions measured with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {7},
   Pages = {2895},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-2895-2},
   Abstract = {A measurement is presented of the [Formula: see text]
             production cross section at [Formula: see text] = 7 TeV
             using [Formula: see text] collision data corresponding to an
             integrated luminosity of 383 [Formula: see text], collected
             with the ATLAS experiment at the LHC. Selection of [Formula:
             see text](1020) mesons is based on the identification of
             charged kaons by their energy loss in the pixel detector.
             The differential cross section is measured as a function of
             the transverse momentum, [Formula: see text], and rapidity,
             [Formula: see text], of the [Formula: see text](1020) meson
             in the fiducial region 500 [Formula: see text] 1200 MeV,
             [Formula: see text] 0.8, kaon [Formula: see text] 230 MeV
             and kaon momentum [Formula: see text] 800 MeV. The
             integrated [Formula: see text]-meson production cross
             section in this fiducial range is measured to be [Formula:
             see text] = 570 [Formula: see text] 8 (stat) [Formula: see
             text] 66 (syst) [Formula: see text] 20 (lumi) [Formula: see
             text].},
   Doi = {10.1140/epjc/s10052-014-2895-2},
   Key = {fds310385}
}

@article{fds362572,
   Author = {Assamagan, K and Chen, C-Y and Chou, JP and Curtin, D and Fedderke, MA and Gershtein, Y and He, X-G and Klute, M and Kozaczuk, J and Kotwal, A and Lowette, S and No, JM and Plehn, T and Qian, J and Ramsey-Musolf, M and Safonov, A and Shelton, J and Spannowsky, M and Su, S and Walker, DGE and Willocq, S and Winslow, P},
   Title = {The Higgs Portal and Cosmology},
   Year = {2016},
   Month = {April},
   Abstract = {Higgs portal interactions provide a simple mechanism for
             addressing two open problems in cosmology: dark matter and
             the baryon asymmetry. In the latter instance, Higgs portal
             interactions may contain the ingredients for a strong first
             order electroweak phase transition as well as new
             CP-violating interactions as needed for electroweak
             baryogenesis. These interactions may also allow for a viable
             dark matter candidate. We survey the opportunities for
             probing the Higgs portal as it relates to these questions in
             cosmology at the LHC and possible future
             colliders.},
   Key = {fds362572}
}

@article{fds332353,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon,
             TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
             VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
             F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings Crépé-Renaudin and MAC and Cutts,
             D and Davis, GA and Davis, K and De, K and De Jong and SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV},
   Title = {The inclusive jet cross section in pp̄ collisions at √s =
             1.8 TeV using the k⊥ algorithm},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {525},
   Number = {3-4},
   Pages = {211-218},
   Publisher = {Elsevier BV},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1016/S0370-2693(01)01441-1},
   Abstract = {The central inclusive jet cross section has been measured
             using a successive-combination algorithm for reconstruction
             of jets. The measurement uses 87.3 pb-1 of data collected
             with the DØ detector at the Fermilab Tevatron pp̄ Collider
             during 1994-1995. The cross section, reported as a function
             of transverse momentum (pT > 60 GeV) in the central region
             of pseudorapidity (|η| < 0.5), exhibits reasonable
             agreement with next-to-leading order QCD predictions, except
             at low pT where the agreement is marginal.},
   Doi = {10.1016/S0370-2693(01)01441-1},
   Key = {fds332353}
}

@article{fds321083,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
             EB and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner,
             M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji,
             W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
             I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
             E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito,
             L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont,
             AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
   Title = {The performance of the jet trigger for the ATLAS detector
             during 2011 data taking.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {10},
   Pages = {526},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4325-0},
   Abstract = {The performance of the jet trigger for the ATLAS detector at
             the LHC during the 2011 data taking period is described.
             During 2011 the LHC provided proton-proton collisions with a
             centre-of-mass energy of 7 TeV and heavy ion collisions
             with a 2.76 TeV per nucleon-nucleon collision energy. The
             ATLAS trigger is a three level system designed to reduce the
             rate of events from the 40 MHz nominal maximum bunch
             crossing rate to the approximate 400 Hz which can be
             written to offline storage. The ATLAS jet trigger is the
             primary means for the online selection of events containing
             jets. Events are accepted by the trigger if they contain one
             or more jets above some transverse energy threshold. During
             2011 data taking the jet trigger was fully efficient for
             jets with transverse energy above 25 GeV for triggers
             seeded randomly at Level 1. For triggers which require a jet
             to be identified at each of the three trigger levels, full
             efficiency is reached for offline jets with transverse
             energy above 60 GeV. Jets reconstructed in the final
             trigger level and corresponding to offline jets with
             transverse energy greater than 60 GeV, are reconstructed
             with a resolution in transverse energy with respect to
             offline jets, of better than 4 % in the central region and
             better than 2.5 % in the forward direction.},
   Doi = {10.1140/epjc/s10052-016-4325-0},
   Key = {fds321083}
}

@article{fds375847,
   Author = {Kotwal, AV},
   Title = {The precision measurement of the W boson mass and its impact
             on physics},
   Journal = {Nature Reviews Physics},
   Volume = {6},
   Number = {3},
   Pages = {180-193},
   Publisher = {Springer Science and Business Media LLC},
   Year = {2024},
   Month = {March},
   url = {http://dx.doi.org/10.1038/s42254-023-00682-0},
   Abstract = {As a mediator of the weak nuclear force, the W boson
             influences many properties of fundamental particles and
             their interactions. Understanding the W boson as accurately
             as possible, including knowing its mass, has been a priority
             in particle physics for decades. In the past few years, in a
             succession of increasing-precision measurements by multiple
             experiments, a significant tension between the measured and
             predicted mass has been documented by the CDF Collaboration.
             Furthermore, smaller differences between different
             measurements exist. Because the W boson mass provides a
             window on new physics, a comparison between different
             measurement techniques can inform the path to further
             investigations. This Perspective article overviews the role
             of the W boson mass in the Standard Model of Particle
             Physics and its extensions, compares and contrasts its
             measurement techniques and discusses prospects and future
             directions.},
   Doi = {10.1038/s42254-023-00682-0},
   Key = {fds375847}
}

@article{fds308106,
   Author = {Abazov, VM and Abbott, B and Abolins, M and Acharya, BS and Adams, DL and Adams, M and Adams, T and Agelou, M and Agram, JL and Ahmed, SN and Ahn,
             SH and Ahsan, M and Alexeev, GD and Alkhazov, G and Alton, A and Alverson,
             G and Alves, GA and Anastasoaie, M and Andeen, T and Anderson, JT and Anderson, S and Andrieu, B and Angstadt, R and Anosov, V and Arnoud, Y and Arov, M and Askew, A and Åsman, B and Assis Jesus and ACS and Atramentov,
             O and Autermann, C and Avila, C and Babukhadia, L and Bacon, TC and Badaud,
             F and Baden, A and Baffioni, S and Bagby, L and Baldin, B and Balm, PW and Banerjee, P and Banerjee, S and Barberis, E and Bardon, O and Barg, W and Bargassa, P and Baringer, P and Barnes, C and Barreto, J and Bartlett,
             JF and Bassler, U and Bhattacharjee, M and Baturitsky, MA and Bauer, D and Bean, A and Baumbaugh, B and Beauceron, S and Begalli, M and Beaudette,
             F and Begel, M and Bellavance, A and Beri, SB and Bernardi, G and Bernhard,
             R and Bertram, I and Besançon, M and Besson, A and Beuselinck, R and Beutel, D and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Binder, M and Biscarat, C and Bishoff, A and Black, KM and Blackler, I and Blazey, G and Blekman, F and Blessing, S and Bloch, D and Blumenschein, U and Bockenthien, E and Bodyagin, V and Boehnlein, A and Boeriu, O and Bolton, TA and Bonamy, P and Bonifas, D and Borcherding, F and Borissov,
             G and Bos, K and Bose, T and Boswell, C and Bowden, M and Brandt, A and Briskin, G and Brock, R and Brooijmans, G and Bross,
             A},
   Title = {The upgraded DØ detector},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {565},
   Number = {2},
   Pages = {463-537},
   Publisher = {Elsevier BV},
   Year = {2006},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.nima.2006.05.248},
   Abstract = {The DØ experiment enjoyed a very successful data-collection
             run at the Fermilab Tevatron collider between 1992 and 1996.
             Since then, the detector has been upgraded to take advantage
             of improvements to the Tevatron and to enhance its physics
             capabilities. We describe the new elements of the detector,
             including the silicon microstrip tracker, central fiber
             tracker, solenoidal magnet, preshower detectors, forward
             muon detector, and forward proton detector. The
             uranium/liquid-argon calorimeters and central muon detector,
             remaining from Run I, are discussed briefly. We also present
             the associated electronics, triggering, and data acquisition
             systems, along with the design and implementation of
             software specific to DØ. © 2006 Elsevier B.V. All rights
             reserved.},
   Doi = {10.1016/j.nima.2006.05.248},
   Key = {fds308106}
}

@article{fds326606,
   Author = {Kotwal, AV},
   Title = {The W Boson mass measurement},
   Volume = {26},
   Pages = {185-200},
   Booktitle = {The Standard Theory of Particle Physics: Essays to Celebrate
             CERN's 60th Anniversary},
   Publisher = {World Scientific},
   Year = {2016},
   Month = {October},
   ISBN = {9789814733502},
   url = {http://dx.doi.org/10.1142/9878},
   Abstract = {The measurement of the W boson mass has been growing in
             importance as its precision has improved, along with the
             precision of other electroweak observables and the top quark
             mass. Over the last decade, the measurement of the W boson
             mass has been led at hadron colliders. Combined with the
             precise measurement of the top quark mass at hadron
             colliders, the W boson mass helped to pin down the mass of
             the Standard Model Higgs boson through its induced radiative
             correction on theW boson mass. With the discovery of the
             Higgs boson and the measurement of its mass, the electroweak
             sector of the Standard Model is over-constrained. Increasing
             the precision of the W boson mass probes new physics at the
             TeV-scale. We summarize an extensive Tevatron (1984-2011)
             program to measure the W boson mass at the CDF and DØ
             experiments. We highlight the recent Tevatron measurements
             and prospects for the final Tevatron measurements.},
   Doi = {10.1142/9878},
   Key = {fds326606}
}

@article{fds346212,
   Author = {Prakash, J and Kotwal, A and Prabhu, H},
   Title = {Therapeutic and prophylactic utility of the memory-enhancing
             drug donepezil hydrochloride on cognition of patients
             undergoing electroconvulsive therapy: a randomized
             controlled trial.},
   Journal = {The journal of ECT},
   Volume = {22},
   Number = {3},
   Pages = {163-168},
   Year = {2006},
   Month = {September},
   url = {http://dx.doi.org/10.1097/01.yct.0000230365.81368.2d},
   Abstract = {<h4>Objectives</h4>Substantial progress has been made in
             identifying how the treatment parameters used in
             electroconvulsive therapy (ECT) impact its cognitive side
             effects. However, there is limited information regarding the
             role of memory enhancers in post-ECT cognitive disturbances.
             We evaluated the therapeutic and prophylactic efficacy of
             the memory-enhancing drug donepezil hydrochloride on
             cognition of patients undergoing ECT.<h4>Methods</h4>A
             triple blind (the study subjects, clinician assessing the
             cognition, and the data analyst were unaware of subject
             allocation for trial assessment) randomized controlled trial
             was carried out in a General Hospital Psychiatry Unit.
             Subjects were randomized into 2 groups. One group received
             ECT with placebo, whereas the other group received ECT and
             donepezil (a memory-enhancing drug). Study participants were
             assessed in post-ECT period to analyze cognitive deficits
             and to compare the differences in 2 groups, as regards
             recovery of various aspects of cognition.<h4>Results</h4>The
             post-ECT recovery of various components of cognition was
             more rapid in patients using donepezil as compared to those
             not given donepezil (P < 0.05).<h4>Conclusions</h4>This
             significant improvement in recovery time among patients
             receiving donepezil bears therapeutic implication in
             immediate post-ECT cognitive deficits.},
   Doi = {10.1097/01.yct.0000230365.81368.2d},
   Key = {fds346212}
}

@article{fds308264,
   Author = {O'Donnell, JM and Kotwal, A and Fortune, HT},
   Title = {Three-state mixing among 0+ states in even Cd
             isotopes.},
   Journal = {Physical review. C, Nuclear physics},
   Volume = {38},
   Number = {5},
   Pages = {2047-2051},
   Year = {1988},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevc.38.2047},
   Abstract = {Ratios of (t,p) transfer intensities to 0+ states in the
             cadmium isotopes have been analyzed using a three-state
             mixing model. The data allows determination of the degree of
             mixing of the rotational (intruder) state into the
             zero-phonon and two-phonon 0+ states. The three lowest 0+
             states are found to be relatively pure and the intruder
             state lies above the two-phonon state in the heavier
             isotopes. © 1988 The American Physical Society.},
   Doi = {10.1103/physrevc.38.2047},
   Key = {fds308264}
}

@article{fds313583,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel,
             A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet,
             NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
             Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
             R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini,
             I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and El Moursli and RC and Chernyatin,
             V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Time-dependent angular analysis of the decay
             Bs0J/ψφ and
             extraction of ΔΓs and the
             CP-violating weak phase φs by
             ATLAS},
   Journal = {JOURNAL OF HIGH ENERGY PHYSICS},
   Volume = {2012},
   Number = {12},
   Year = {2012},
   ISSN = {1126-6708},
   url = {http://dx.doi.org/10.1007/JHEP12(2012)072},
   Abstract = {A measurement of B0s → J /ψφ decay parameters, including
             the CP -violating weak phase φ s and the decay width
             difference ΔΓ s is reported, using 4.9 fb-1 of integrated
             luminosity collected in 2011 by the ATLAS detector from LHC
             pp collisions at a centre-of-mass energy √s = 7 TeV. The
             mean decay width Γ s and the transversity amplitudes |A
             0(0)|2 and |A arap;(0)|2 are also measured. The values
             reported for these parameters are: φs = 0.22 ± 0.41 (stat)
             ± 0.10 (syst) rad} ΔΓ s = 0.053 ± 0.021 (stat) ± 0.010
             (sast) ps-1 Γ s = 0.677 ± 0.007 (stat) ± 0.004 (sast)
             ps-1 |A0(0)|2 = 0.528 ± 0.006 (stat) ± 0.009 (sast)
             |A0(0)|2 = 0.220 ± 0.008 (stat) ± 0.007 (sast) where the
             values quoted for φ s and ΔΓ s correspond to the solution
             compatible with the external measurements to which the
             strong phase δ ⊥ is constrained and where ΔΓ s is
             constrained to be positive. The fraction of S-wave KK or f 0
             contamination through the decays B0s→ J /ψK +
             K-}}\left({{f-0}} \right)}} \right.} is measured as well and
             is found to be consistent with zero. Results for φ s and
             ΔΓ s are also presented as 68%, 90% and 95% likelihood
             contours, which show agreement with Standard Model
             expectations.[Figure not available: see fulltext.] © 2012
             CERN for the benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP12(2012)072},
   Key = {fds313583}
}

@article{fds375336,
   Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
             J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
             SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Aly, M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
             CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
   Title = {Tools for estimating fake/non-prompt lepton backgrounds with
             the ATLAS detector at the LHC},
   Journal = {Journal of Instrumentation},
   Volume = {18},
   Number = {11},
   Pages = {T11004-T11004},
   Publisher = {IOP Publishing},
   Year = {2023},
   Month = {November},
   url = {http://dx.doi.org/10.1088/1748-0221/18/11/T11004},
   Abstract = {Measurements and searches performed with the ATLAS detector
             at the CERN LHC often involve signatures with one or more
             prompt leptons. Such analyses are subject to
             'fake/non-prompt' lepton backgrounds, where either a hadron
             or a lepton from a hadron decay or an electron from a photon
             conversion satisfies the prompt-lepton selection criteria.
             These backgrounds often arise within a hadronic jet because
             of particle decays in the showering process, particle
             misidentification or particle interactions with the detector
             material. As it is challenging to model these processes with
             high accuracy in simulation, their estimation typically uses
             data-driven methods. Three methods for carrying out this
             estimation are described, along with their implementation in
             ATLAS and their performance.},
   Doi = {10.1088/1748-0221/18/11/T11004},
   Key = {fds375336}
}

@article{fds308098,
   Author = {Abulencia, and A, and others},
   Title = {Top quark mass measurement from dilepton events at CDF
             II},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {15},
   Pages = {152002},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.152002},
   Abstract = {We report a measurement of the top quark mass using events
             collected by the CDF II Detector from p anti-p collisions at
             s**(1/2) = 1.96 TeV at the Fermilab Tevatron. We calculate a
             likelihood function for the top mass in events that are
             consistent with t anti-t --> b-bar l- nu-bar_l bl'+ nu'_l
             decays. The likelihood is formed as the convolution of the
             leading-order matrix element and detector resolution
             functions. The joint likelihood is the product of
             likelihoods for each of 33 events collected in 340 pb-1 of
             integrated luminosity, yielding a top quark mass M_t = 165.2
             +/- 6.1(stat.) +/- 3.4(syst.) GeV/c2. This first application
             of a matrix-element technique to tt-bar --> bl+ nu_l b-bar
             l'- nu-bar_l' decays gives the most precise single
             measurement of M_t in dilepton events. Combined with other
             CDF Run II measurements using dilepton events, we measure
             M_t = 167.9 +/- 5.2(stat.) +/- 3.7(syst.)
             GeV/c2.},
   Doi = {10.1103/physrevlett.96.152002},
   Key = {fds308098}
}

@article{fds308121,
   Author = {Abulencia, and A, and others},
   Title = {Top quark mass measurement from dilepton events at CDF II
             with the matrix-element method},
   Journal = {Phys. Rev.},
   Volume = {D74},
   Number = {3},
   Pages = {032009},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.74.032009},
   Abstract = {We describe a measurement of the top quark mass using events
             with two charmed leptons collected by the CDF II detector
             from p anti-p collisions with s**(1/2) = 1.96 TeV at the
             Fermilab Tevatron. The likelihood in top mass is calculated
             for each event by convoluting the leading order matrix
             element describing qqbar --> t anti-t --> b l nu_l b-bar l'
             nu_l' with detector resolution functions. The presence of
             background events in the data sample is modeled using
             similar calculations involving the matrix elements for major
             background processes. In a data sample with integrated
             luminosity of 340 pb-1, we observe 33 candidate events and
             measure M_top = 165.2 +/- 6.1(stat.) +/- 3.4(syst.) GeV/c2.
             This measurement represents the first application of this
             method to events with two charged leptons and is the most
             precise single measurement of the top quark mass in this
             channel.},
   Doi = {10.1103/PhysRevD.74.032009},
   Key = {fds308121}
}

@article{fds307894,
   Author = {Aaltonen, and T, and others},
   Title = {Top Quark Mass Measurement in the $lepton+jets$ Channel
             Using a Matrix Element Method and in situ Jet Energy
             Calibration},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {25},
   Pages = {252001},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.252001},
   Abstract = {A precision measurement of the top quark mass m(t) is
             obtained using a sample of tt events from pp collisions at
             the Fermilab Tevatron with the CDF II detector. Selected
             events require an electron or muon, large missing transverse
             energy, and exactly four high-energy jets, at least one of
             which is tagged as coming from a b quark. A likelihood is
             calculated using a matrix element method with quasi-Monte
             Carlo integration taking into account finite detector
             resolution and jet mass effects. The event likelihood is a
             function of m(t) and a parameter Δ(JES) used to calibrate
             the jet energy scale in situ. Using a total of 1087 events
             in 5.6 fb(-1) of integrated luminosity, a value of
             m(t)=173.0 ± 1.2 GeV/c(2) is measured.},
   Doi = {10.1103/PhysRevLett.105.252001},
   Key = {fds307894}
}

@article{fds307980,
   Author = {Aaltonen, T and others},
   Title = {Top quark mass measurement in the lepton plus jets channel
             using a modified matrix element method},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {7},
   Pages = {072001},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.072001},
   Abstract = {We report a measurement of the top quark mass, mt, obtained
             from pp̄ collisions at s=1.96TeV at the Fermilab Tevatron
             using the CDF II detector. We analyze a sample corresponding
             to an integrated luminosity of 1.9fb-1. We select events
             with an electron or muon, large missing transverse energy,
             and exactly four high-energy jets in the central region of
             the detector, at least one of which is tagged as coming from
             a b quark. We calculate a signal likelihood using a matrix
             element integration method, where the matrix element is
             modified by using effective propagators to take into account
             assumptions on event kinematics. Our event likelihood is a
             function of mt and a parameter JES (jet energy scale) that
             determines in situ the calibration of the jet energies. We
             use a neural network discriminant to distinguish signal from
             background events. We also apply a cut on the peak value of
             each event likelihood curve to reduce the contribution of
             background and badly reconstructed events. Using the 318
             events that pass all selection criteria, we find
             mt=172.7±1.8(stat+JES) ±1.2(syst)GeV/c2. © 2009 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.79.072001},
   Key = {fds307980}
}

@article{fds307979,
   Author = {Aaltonen, T and others},
   Title = {Top quark mass measurement in the tt̅ all hadronic channel
             using a matrix element technique in pp̅ collisions at
             sqrt[s] =1.96 TeV},
   Journal = {Physical Review D},
   Volume = {79},
   Number = {7},
   Pages = {072010},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.072010},
   Abstract = {We present a measurement of the top quark mass in the all
             hadronic channel (tt̅ →bb̅ q1q̅ 2q3q̅ 4) using
             943  pb-1 of pp̅ collisions at sqrt[s]=1.96  TeV
             collected at the CDF II detector at Fermilab (CDF). We apply
             the standard model production and decay matrix element (ME)
             to tt̅ candidate events. We calculate per-event probability
             densities according to the ME calculation and construct
             template models of signal and background. The scale of the
             jet energy is calibrated using additional templates formed
             with the invariant mass of pairs of jets. These templates
             form an overall likelihood function that depends on the top
             quark mass and on the jet energy scale (JES). We estimate
             both by maximizing this function. Given 72 observed events,
             we measure a top quark mass of 171.1 &plusmn; 3.7(stat+JES)
             &plusmn; 2.1(syst)  GeV/c2. The combined uncertainty on
             the top quark mass is 4.3  GeV/c2.},
   Doi = {10.1103/PhysRevD.79.072010},
   Key = {fds307979}
}

@article{fds307925,
   Author = {Aaltonen, and T, and others},
   Title = {Top Quark Mass Measurement using $m_{T2}$ in the Dilepton
             Channel at CDF},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {3},
   Pages = {031102},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.031102},
   Abstract = {http://arxiv.org/abs/0911.2956},
   Doi = {10.1103/PhysRevD.81.031102},
   Key = {fds307925}
}

@article{fds307869,
   Author = {Aaltonen, and T, and al, E},
   Title = {Top quark mass measurement using the template method at
             {CDF}},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {11},
   Pages = {111101},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.111101},
   Abstract = {We present a measurement of the top quark mass in the
             lepton+jets and dilepton channels of tt̄ decays using the
             data sample corresponding to an integrated luminosity of
             5.6fb-1 of pp̄ collisions at Tevatron with √s=1.96TeV,
             collected with the CDF II detector. We construct templates
             of two reconstructed top quark masses from different
             jets-to-quarks combinations and the invariant mass of two
             jets from the W decays in the lepton+jets channel, and a
             reconstructed top quark mass and mT2, a variable related to
             the transverse mass in events with two missing particles, in
             the dilepton channel. The simultaneous fit of the templates
             from signal and background events in the lepton+jets and
             dilepton channels to the data yields a measured top quark
             mass of Mtop=172.1±1.1(stat)±0. 9(syst)GeV/c2. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.83.111101},
   Key = {fds307869}
}

@article{fds308107,
   Author = {Abulencia, and A, and others},
   Title = {Top quark mass measurement using the template method in the
             lepton + jets channel at CDF II},
   Journal = {Phys. Rev.},
   Volume = {D73},
   Number = {3},
   Pages = {032003},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.032003},
   Abstract = {This article presents a measurement of the top quark mass
             using the CDF II detector at Fermilab. Colliding beams of
             protons and anti-protons at Fermilab's Tevatron (s**(1/2) =
             1.96 TeV) produce top/anti-top pairs, which decay to W+ W-
             bb-bar; events are selected where one W decays to hadrons,
             and the other W decays to either e or mu plus a neutrino.
             The data sample corresponds to an integrated luminosity of
             approximately 318 pb-1. A total of 165 tt-bar events are
             separated into four subsamples based on jet transverse
             energy thresholds and the number of b jets identified by
             reconstructing a displaced vertex. In each event, the
             reconstructed top quark invariant mass is determined by
             minimizing a chi2 for the overconstrained kinematic system.
             At the same time, the mass of the hadronically decaying W
             boson is measured in the same event sample. The observed W
             boson mass provides an in situ improvement in the
             determination of the hadronic jet energy scale, JES. A
             simultaneous likelihood fit of the reconstructed top quark
             masses and the W boson invariant masses in the data sample
             to distributions from simulated signal and background events
             gives a top quark mass of 173.5+3.7_-3.6(stat. + JES) +/-
             1.3 (other syst.) GeV/c2, or 173.5+3.9_-3.8
             GeV/c2.},
   Doi = {10.1103/PhysRevD.73.032003},
   Key = {fds308107}
}

@article{fds307592,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Top-quark mass measurement in events with jets and missing
             transverse energy using the full CDF data
             set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.011101},
   Abstract = {We present a measurement of the top-quark mass using the
             full data set of Tevatron √s=1.96 TeV proton-antiproton
             collisions recorded by the CDF II detector, corresponding to
             an integrated luminosity of 8.7 fb-1. The analysis uses
             events with one semileptonic t or t̄ decay, but without
             detection of the electron or muon. We select events with
             significant missing transverse energy and multiple jets. We
             veto events containing identified electrons or muons. We
             obtain distributions of the top-quark masses and the
             invariant mass of the two jets from W-boson decays from data
             and compare these to templates derived from signal and
             background samples to extract the top-quark mass and the
             energy scale of the calorimeter jets with in situ
             calibration. A likelihood fit of the templates from signal
             and background events to the data yields the top-quark mass,
             Mtop=173.93±1.64(stat)±0. 87(syst) GeV/c2. This result is
             the most precise measurement to date of the mass of the top
             quark in this event topology. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.88.011101},
   Key = {fds307592}
}

@article{fds356739,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
             F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Top-quark mass measurement in the all-hadronic tt¯ decay
             channel at √s=8 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2017},
   Number = {9},
   Year = {2017},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2017)118},
   Abstract = {The top-quark mass is measured in the all-hadronic
             top-antitop quark decay channel using proton-proton
             collisions at a centre-of-mass energy of s=8 TeV with the
             ATLAS detector at the CERN Large Hadron Collider. The data
             set used in the analysis corresponds to an integrated
             luminosity of 20.2 fb −1 . The large multi-jet background
             is modelled using a data-driven method. The top-quark mass
             is obtained from template fits to the ratio of the three-jet
             to the dijet mass. The three-jet mass is obtained from the
             three jets assigned to the top quark decay. From these three
             jets the dijet mass is obtained using the two jets assigned
             to the W boson decay. The top-quark mass is measured to be
             173.72 ± 0.55 (stat.) ± 1.01 (syst.) GeV.[Figure not
             available: see fulltext.].},
   Doi = {10.1007/JHEP09(2017)118},
   Key = {fds356739}
}

@article{fds307831,
   Author = {Aaltonen, TEA},
   Title = {Top-Quark Mass Measurement Using Events with Missing
             Transverse Energy and Jets at CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {23},
   Pages = {232002},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.232002},
   Abstract = {We present a measurement of the top-quark mass using a
             sample of $t\bar{t}$ events in 5.7  fb-1 of integrated
             luminosity from $p\bar{p}$ collisions at the Fermilab
             Tevatron with $\sqrt{s}=1.96$  TeV and collected by the
             CDF II Detector. We select events having large missing
             transverse energy, and four, five, or six jets with at least
             one jet tagged as coming from a b quark, and reject events
             with identified charged leptons. This analysis considers
             events from the semileptonic tt̅ decay channel, including
             events that contain tau leptons. The measurement is based on
             a multidimensional template method. We fit the data to
             signal templates of varying top-quark masses and background
             templates, and measure a top-quark mass of Mtop=$172.32\pm
             2.4$(stat)$\pm 1.0$(syst)  GeV/c2.},
   Doi = {10.1103/PhysRevLett.107.232002},
   Key = {fds307831}
}

@article{fds347509,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa,
             M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton,
             AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates,
             RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer,
             F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin,
             PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker,
             M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
             JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford,
             L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister,
             I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
             JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio,
             D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet,
             S and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans,
             RC and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez,
             VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman,
             JD and Charlton, DG and Chau, CC and Barajas, CAC and Che, S and Cheatham,
             S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
             S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn,
             AP},
   Title = {Topological cell clustering in the ATLAS calorimeters and
             its performance in LHC Run 1.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {77},
   Number = {7},
   Pages = {490},
   Year = {2017},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-017-5004-5},
   Abstract = {The reconstruction of the signal from hadrons and jets
             emerging from the proton-proton collisions at the Large
             Hadron Collider (LHC) and entering the ATLAS calorimeters is
             based on a three-dimensional topological clustering of
             individual calorimeter cell signals. The cluster formation
             follows cell signal-significance patterns generated by
             electromagnetic and hadronic showers. In this, the
             clustering algorithm implicitly performs a topological noise
             suppression by removing cells with insignificant signals
             which are not in close proximity to cells with significant
             signals. The resulting <i>topological cell clusters</i> have
             shape and location information, which is exploited to apply
             a local energy calibration and corrections depending on the
             nature of the cluster. Topological cell clustering is
             established as a well-performing calorimeter signal
             definition for jet and missing transverse momentum
             reconstruction in ATLAS.},
   Doi = {10.1140/epjc/s10052-017-5004-5},
   Key = {fds347509}
}

@article{fds346206,
   Author = {Priya, R and Kotwal, A and Qadeer, I},
   Title = {Toward an ecosocial epidemiological approach to goiter and
             other iodine deficiency disorders: a case study of India's
             technocratic program for universal iodization of
             salt.},
   Journal = {International journal of health services : planning,
             administration, evaluation},
   Volume = {39},
   Number = {2},
   Pages = {343-362},
   Year = {2009},
   Month = {January},
   url = {http://dx.doi.org/10.2190/hs.39.2.g},
   Abstract = {The program of universal salt iodization (USI) was
             intensified in the 1990s. Unfortunately, a recent World
             Health Organization review finds that there was a global
             increase of 31.7 percent in total goiter rate from 1993 to
             2003. However, the WHO review places only 1 country as
             severely, 13 as moderately, and 40 as mildly deficient in
             populations' iodine nutrition, and places 43 countries at
             optimal, 24 at high, and 5 at excessive levels of iodine
             nutrition. Thus, it is imperative to weigh the benefits and
             risks of intensifying USI further. The WHO review places
             India in the category of "adequate" iodine nutrition, but in
             2005 the Government of India promulgated a universal ban on
             sale of non-iodized salt, calling iodine deficiency
             disorders (IDDs) a major public health problem. This article
             attempts to understand these contradictions and weigh the
             benefits and costs of USI. Based on a review of studies
             since the 1920s, the authors reconstruct the evolution of
             IDD control in India. Conceptual and methodological
             limitations challenge the evidence base and rationale of
             stricter implementation of USI now. Finding evidence for its
             negative impact, the authors recommend a reexamination of
             the USI strategy and propose a safer, people-centered,
             ecosocial epidemiological approach rather than a universal
             legal ban.},
   Doi = {10.2190/hs.39.2.g},
   Key = {fds346206}
}

@article{fds346188,
   Author = {Kotwal, A},
   Title = {Training-associated injuries among Armed Forces
             trainees.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {68},
   Number = {2},
   Pages = {106-107},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1016/s0377-1237(12)60015-x},
   Doi = {10.1016/s0377-1237(12)60015-x},
   Key = {fds346188}
}

@article{fds356552,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
             L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
             T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Pozo, JAA and Bella, LA and Araque, JP and Ferraz, VA and Pereira,
             RA and Arcangeletti, C and Arce, ATH and Arduh, FA},
   Title = {Transverse momentum and process dependent azimuthal
             anisotropies in √sNN=8.16 TeV p+Pb collisions with the
             ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {80},
   Number = {1},
   Year = {2020},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-020-7624-4},
   Abstract = {The azimuthal anisotropy of charged particles produced in
             sNN=8.16 TeV p+Pb collisions is measured with the ATLAS
             detector at the LHC. The data correspond to an integrated
             luminosity of 165 nb - 1 that was collected in 2016.
             Azimuthal anisotropy coefficients, elliptic v2 and
             triangular v3, extracted using two-particle correlations
             with a non-flow template fit procedure, are presented as a
             function of particle transverse momentum (pT) between 0.5
             and 50 GeV. The v2 results are also reported as a function
             of centrality in three different particle pT intervals. The
             results are reported from minimum-bias events and
             jet-triggered events, where two jet pT thresholds are used.
             The anisotropies for particles with pT less than about
             2 GeV are consistent with hydrodynamic flow expectations,
             while the significant non-zero anisotropies for pT in the
             range 9–50 GeV are not explained within current
             theoretical frameworks. In the pT range 2–9 GeV, the
             anisotropies are larger in minimum-bias than in
             jet-triggered events. Possible origins of these effects,
             such as the changing admixture of particles from hard
             scattering and the underlying event, are
             discussed.},
   Doi = {10.1140/epjc/s10052-020-7624-4},
   Key = {fds356552}
}

@article{fds307811,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'errico, M},
   Title = {Transverse momentum cross section of e +e
             - pairs in the Z-boson region from pp̄
             collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.052010},
   Abstract = {The transverse momentum cross section of e +e - pairs in the
             Z-boson mass region of 66-116GeV/c2 is precisely measured
             using Run II data corresponding to 2.1fb -1 of integrated
             luminosity recorded by the Collider Detector at Fermilab.
             The cross section is compared with two quantum chromodynamic
             calculations. One is a fixed-order perturbative calculation
             at O(αs2), and the other combines perturbative predictions
             at high transverse momentum with the gluon resummation
             formalism at low transverse momentum. Comparisons of the
             measurement with calculations show reasonable agreement. The
             measurement is of sufficient precision to allow refinements
             in the understanding of the transverse momentum
             distribution. © 2012 American Physical Society.},
   Doi = {10.1103/PhysRevD.86.052010},
   Key = {fds307811}
}

@article{fds321072,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov,
             A},
   Title = {Transverse momentum, rapidity, and centrality dependence of
             inclusive charged-particle production in sNN=5.02
             TeV p + Pb collisions measured by the ATLAS
             experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {763},
   Pages = {313-336},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.10.053},
   Abstract = {Measurements of the per-event charged-particle yield as a
             function of the charged-particle transverse momentum and
             rapidity are performed using p+Pb collision data collected
             by the ATLAS experiment at the LHC at a centre-of-mass
             energy of sNN=5.02TeV. Charged particles are reconstructed
             over pseudorapidity |η|<2.3 and transverse momentum between
             0.1 GeV and 22 GeV in a dataset corresponding to an
             integrated luminosity of 1 μb−1. The results are
             presented in the form of charged-particle nuclear
             modification factors, where the p+Pb charged-particle
             multiplicities are compared between central and peripheral
             p+Pb collisions as well as to charged-particle cross
             sections measured in pp collisions. The p+Pb collision
             centrality is characterized by the total transverse energy
             measured in −4.9<η<−3.1, which is in the direction of
             the outgoing lead beam. Three different estimations of the
             number of nucleons participating in the p+Pb collision are
             carried out using the Glauber model and two Glauber–Gribov
             colour-fluctuation extensions to the Glauber model. The
             values of the nuclear modification factors are found to vary
             significantly as a function of rapidity and transverse
             momentum. A broad peak is observed for all centralities and
             rapidities in the nuclear modification factors for
             charged-particle transverse momentum values around 3 GeV.
             The magnitude of the peak increases for more central
             collisions as well as rapidity ranges closer to the
             direction of the outgoing lead nucleus.},
   Doi = {10.1016/j.physletb.2016.10.053},
   Key = {fds321072}
}

@article{fds316849,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Triggers for displaced decays of long-lived neutral
             particles in the ATLAS detector},
   Journal = {Journal of Instrumentation},
   Volume = {8},
   Number = {7},
   Pages = {P07015-P07015},
   Publisher = {IOP Publishing},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1748-0221/8/07/P07015},
   Abstract = {A set of three dedicated triggers designed to detect
             long-lived neutral particles decaying throughout the ATLAS
             detector to a pair of hadronic jets is described. The
             efficiencies of the triggers for selecting displaced decays
             as a function of the decay position are presented for
             simulated events. The effect of pile-up interactions on the
             trigger efficiencies and the dependence of the trigger rate
             on instantaneous luminosity during the 2012 data-taking
             period at the LHC are discussed.},
   Doi = {10.1088/1748-0221/8/07/P07015},
   Key = {fds316849}
}

@article{fds332351,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Balamurali, V and Baldin,
             B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer,
             P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat,
             PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Bolton, TA and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
             F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chang, SM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cretsinger, C and Cummings, MAC and Cutts, D and Davis, GA and De, K and de Jong, SJ and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov,
             SP},
   Title = {tt̄ production cross section in pp̄ collisions at √s =
             1.8 TeV},
   Journal = {Physical Review D},
   Volume = {67},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2003},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.67.012004},
   Abstract = {Results are presented on a measurement of the tt̄ pair
             production cross section in pp̄ collisions at √s = 1.8
             TeV from nine independent decay channels. The data were
             collected by the DØ experiment during the 1992-1996 run of
             the Fermilab Tevatron Collider. A total of 80 candidate
             events is observed with an expected background of 38.8±3.3
             events. For a top quark mass of 172.1 GeV/c2, the measured
             cross section is 5.69 ±1.21(stat)±1.04(syst) pb. © 2003
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.67.012004},
   Key = {fds332351}
}

@article{fds346167,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
             O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
             V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
   Title = {Two-particle Bose-Einstein correlations in pp
             collisions at [Formula: see text] 0.9 and 7 TeV measured
             with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {10},
   Pages = {466},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3644-x},
   Abstract = {The paper presents studies of Bose-Einstein Correlations
             (BEC) for pairs of like-sign charged particles measured in
             the kinematic range [Formula: see text] 100 MeV and
             [Formula: see text] 2.5 in proton collisions at
             centre-of-mass energies of 0.9 and 7 TeV with the ATLAS
             detector at the CERN Large Hadron Collider. The integrated
             luminosities are approximately 7 [Formula: see
             text]b[Formula: see text], 190 [Formula: see
             text]b[Formula: see text] and 12.4 nb[Formula: see text]
             for 0.9 TeV, 7 TeV minimum-bias and 7 TeV
             high-multiplicity data samples, respectively. The
             multiplicity dependence of the BEC parameters characterizing
             the correlation strength and the correlation source size are
             investigated for charged-particle multiplicities of up to
             240. A saturation effect in the multiplicity dependence of
             the correlation source size parameter is observed using the
             high-multiplicity 7 TeV data sample. The dependence of the
             BEC parameters on the average transverse momentum of the
             particle pair is also investigated.},
   Doi = {10.1140/epjc/s10052-015-3644-x},
   Key = {fds346167}
}

@article{fds364958,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
             GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez
             Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
             R},
   Title = {Two-particle Bose–Einstein correlations in pp collisions
             at √s=13 TeV measured with the ATLAS detector at the
             LHC},
   Journal = {European Physical Journal C},
   Volume = {82},
   Number = {7},
   Year = {2022},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-022-10472-0},
   Abstract = {This paper presents studies of Bose–Einstein correlations
             (BEC) in proton–proton collisions at a centre-of-mass
             energy of 13 TeV, using data from the ATLAS detector at the
             CERN Large Hadron Collider. Data were collected in a special
             low-luminosity configuration with a minimum-bias trigger and
             a high-multiplicity track trigger, accumulating integrated
             luminosities of 151 μ b- 1 and 8.4 nb- 1, respectively.
             The BEC are measured for pairs of like-sign charged
             particles, each with | η| < 2.5 , for two kinematic ranges:
             the first with particle pT> 100 MeV and the second with
             particle pT> 500 MeV. The BEC parameters, characterizing the
             source radius and particle correlation strength, are
             investigated as functions of charged-particle multiplicity
             (up to 300) and average transverse momentum of the pair (up
             to 1.5 GeV). The double-differential dependence on
             charged-particle multiplicity and average transverse
             momentum of the pair is also studied. The BEC radius is
             found to be independent of the charged-particle multiplicity
             for high charged-particle multiplicity (above 100),
             confirming a previous observation at lower energy. This
             saturation occurs independent of the transverse momentum of
             the pair.},
   Doi = {10.1140/epjc/s10052-022-10472-0},
   Key = {fds364958}
}

@article{fds307797,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {Underlying event characteristics and their dependence on jet
             size of charged-particle jet events in pp collisions at
             √(s)=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.072004},
   Abstract = {Distributions sensitive to the underlying event are studied
             in events containing one or more charged-particle jets
             produced in pp collisions at √s=7TeV with the ATLAS
             detector at the Large Hadron Collider (LHC). These
             measurements reflect 800μb-1 of data taken during 2010.
             Jets are reconstructed using the anti-kt algorithm with
             radius parameter R varying between 0.2 and 1.0.
             Distributions of the charged-particle multiplicity, the
             scalar sum of the transverse momentum of charged particles,
             and the average charged-particle pT are measured as
             functions of pTjet in regions transverse to and opposite the
             leading jet for 4GeV<pTjet<100GeV. In addition, the R
             dependence of the mean values of these observables is
             studied. In the transverse region, both the multiplicity and
             the scalar sum of the transverse momentum at fixed pTjet
             vary significantly with R, while the average
             charged-particle transverse momentum has a minimal
             dependence on R. Predictions from several Monte Carlo tunes
             have been compared to the data; the predictions from Pythia
             6, based on tunes that have been determined using LHC data,
             show reasonable agreement with the data, including the
             dependence on R. Comparisons with other generators indicate
             that additional tuning of soft-QCD parameters is necessary
             for these generators. The measurements presented here
             provide a testing ground for further development of the
             Monte Carlo models. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.86.072004},
   Key = {fds307797}
}

@article{fds346202,
   Author = {Naga Prasad and SV and Duan, Z-H and Gupta, MK and Surampudi, VSK and Volinia, S and Calin, GA and Liu, C-G and Kotwal, A and Moravec, CS and Starling, RC and Perez, DM and Sen, S and Wu, Q and Plow, EF and Croce, CM and Karnik, S},
   Title = {Unique microRNA profile in end-stage heart failure indicates
             alterations in specific cardiovascular signaling
             networks.},
   Journal = {The Journal of biological chemistry},
   Volume = {284},
   Number = {40},
   Pages = {27487-27499},
   Year = {2009},
   Month = {October},
   url = {http://dx.doi.org/10.1074/jbc.m109.036541},
   Abstract = {It is well established that gene expression patterns are
             substantially altered in cardiac hypertrophy and heart
             failure, but the reasons for such differences are not clear.
             MicroRNAs (miRNAs) are short noncoding RNAs that provide a
             novel mechanism for gene regulation. The goal of this study
             was to comprehensively test for alterations in miRNA
             expression using human heart failure samples with an aim to
             build signaling pathway networks using predicted targets for
             the miRNAs and to identify nodal molecules that control
             these networks. Genome-wide profiling of miRNAs was
             performed using custom-designed miRNA microarray followed by
             validation on an independent set of samples. Eight miRNAs
             are significantly altered in heart failure of which we have
             identified two novel miRNAs that are yet to be implicated in
             cardiac pathophysiology. To gain an unbiased global
             perspective on regulation by altered miRNAs, predicted
             targets of eight miRNAs were analyzed using the Ingenuity
             Pathways Analysis network algorithm to build signaling
             networks and identify nodal molecules. The majority of nodal
             molecules identified in our analysis are targets of altered
             miRNAs and are known regulators of cardiovascular signaling.
             A heart failure gene expression data base was used to
             analyze changes in expression patterns for these target
             nodal molecules. Indeed, expression of nodal molecules was
             altered in heart failure and inversely correlated to miRNA
             changes validating our analysis. Importantly, using network
             analysis we have identified a limited number of key
             functional targets that may regulate expression of the
             myriad proteins in heart failure and could be potential
             therapeutic targets.},
   Doi = {10.1074/jbc.m109.036541},
   Key = {fds346202}
}

@article{fds346207,
   Author = {Prakash, J and Singh, PK and Kotwal, A and Ramakrishnan,
             TS},
   Title = {Unknown Poisoning Amongst Serving Personnel.},
   Journal = {Medical journal, Armed Forces India},
   Volume = {65},
   Number = {1},
   Pages = {41-43},
   Year = {2009},
   Month = {January},
   url = {http://dx.doi.org/10.1016/s0377-1237(09)80053-1},
   Abstract = {<h4>Background</h4>Poisoning is recognized as an important
             health problem in many countries of the world. There is
             incomplete information on poisoning accidents, which is a
             major problem in developing countries.<h4>Methods</h4>A
             cross-sectional analysis of hospital records of armed forces
             personnel admitted with a provisional diagnosis of unknown
             poisoning was carried out.<h4>Result</h4>Unknown poisoning
             represented 0.25% of hospital admissions and 6584 man-hours
             were lost. 85% poisonings occurred at railway station and
             majority were food related. Average length of stay in the
             hospital was 14.69 days. Ten patients required intensive
             care and two patients were admitted to the psychiatry
             ward.<h4>Conclusion</h4>Majority of the incidents occurred
             in railways, signifying the importance of health education
             and precaution while proceeding on leave. Since, most of the
             affected were young soldiers, education should start from
             recruiting centers. Few patients had alcohol intoxication
             reflecting their dependence potential and need for
             reinforcing prohibition on alcohol consumption during
             travel.},
   Doi = {10.1016/s0377-1237(09)80053-1},
   Key = {fds346207}
}

@article{fds307933,
   Author = {Aaltonen, and T, and others},
   Title = {Updated search for the flavor-changing neutral-current decay
             $D^{0}\rightarrow{}\mu{}^{+}\mu{}^{-}$ in $pp[over
             \ifmmode\bar\else\textasciimacron\fi{}]$ collisions at
             $\sqrt{s}=1.96$ TeV},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {9},
   Pages = {091105},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.091105},
   Abstract = {We report on a search for the flavor-changing
             neutral-current decay D0→μ⊃+μ⊃- in pp̄ collisions
             at √s=1.96TeV using 360pb⊃-1 of integrated luminosity
             collected by the CDF II detector at the Fermilab Tevatron
             collider. A displaced vertex trigger selects long-lived D0
             candidates in the μ⊃+μ⊃-, π⊃+π⊃-, and
             K⊃-π⊃+ decay modes. We use the Cabibbo-favored
             D0→K⊃- π⊃+ channel to optimize the selection criteria
             in an unbiased manner, and the kinematically similar
             D0→π⊃+π⊃- channel for normalization. We set an upper
             limit on the branching fraction B(D0→μ⊃+μ⊃-)<2.1×10⊃-7(3.0×10⊃-7)
             at the 90% (95%) confidence level. © 2010 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.82.091105},
   Key = {fds307933}
}

@article{fds307634,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Updated search for the standard model Higgs boson in events
             with jets and missing transverse energy using the full CDF
             data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.052008},
   Abstract = {We present an updated search for the Higgs boson produced in
             association with a vector boson in the final state with
             missing transverse energy and two jets. We use the full CDF
             data set corresponding to an integrated luminosity of 9.45
             fb-1 at a proton-antiproton center-of-mass energy of
             √s=1.96 TeV. New to this analysis is the inclusion of a
             b-jet identification algorithm specifically optimized for
             H→bb̄ searches. Across the Higgs boson mass range
             90≤mH≤150 GeV/c2, the expected 95% credibility level
             upper limits on the VH production cross section times the
             H→bb̄ branching fraction are improved by an average of
             14% relative to the previous analysis. At a Higgs boson mass
             of 125 GeV/c2, the observed (expected) limit is 3.06 (3.33)
             times the standard model prediction, corresponding to one of
             the most sensitive searches to date in this final state. ©
             2013 American Physical Society.},
   Doi = {10.1103/PhysRevD.87.052008},
   Key = {fds307634}
}

@article{fds364961,
   Author = {Buarque Franzosi and D and Gallinaro, M and Ruiz, R and Aarrestad, TK and Cetorelli, F and Chiesa, M and Costantini, A and Denner, A and Dittmaier, S and Franken, R and Govoni, P and Han, T and Kotwal, AV and Li,
             J and Lohwasser, K and Long, K and Ma, Y and Mantani, L and Marchegiani, M and Pellen, M and Pelliccioli, G and Potamianos, K and Reuter, J and Schmidt, T and Schwan, C and Szleper, M and Verheyen, R and Xie, K and Zhang, R},
   Title = {Vector boson scattering processes: Status and
             prospects},
   Journal = {Reviews in Physics},
   Volume = {8},
   Year = {2022},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.revip.2022.100071},
   Abstract = {Insight into the electroweak (EW) and Higgs sectors can be
             achieved through measurements of vector boson scattering
             (VBS) processes. The scattering of EW bosons are rare
             processes that are precisely predicted in the Standard Model
             (SM) and are closely related to the Higgs mechanism.
             Modifications to VBS processes are also predicted in models
             of physics beyond the SM (BSM), for example through changes
             to the Higgs boson couplings to gauge bosons and the
             resonant production of new particles. In this review,
             experimental results and theoretical developments of VBS at
             the Large Hadron Collider, its high luminosity upgrade, and
             future colliders are presented.},
   Doi = {10.1016/j.revip.2022.100071},
   Key = {fds364961}
}

@article{fds340914,
   Author = {Thurman Keup and RM and Kotwal, AV and Tecchio, M and Byon Wagner,
             A},
   Title = {W boson physics at hadron colliders},
   Journal = {Reviews of Modern Physics},
   Volume = {73},
   Number = {267},
   Pages = {40},
   Year = {2001},
   Month = {April},
   Abstract = {The use of hadron colliders to investigate the properties of
             the W bosons started in 1982 at the CERN SpS collider. Since
             then, the Tevatron experiments at Fermilab have recorded a
             large sample of W events which allowed precision
             measurements of the properties of W bosons. In this paper
             the authors review W gauge boson physics at hadron colliders
             from 1982 to 2000. They first discuss the production
             mechanism and detection of W bosons in p collisions. After a
             brief review of the early studies, W boson physics at the
             Tevatron collider are thoroughly examined. Finally, possible
             future directions of W boson physics at hadron colliders are
             discussed.},
   Key = {fds340914}
}

@article{fds308193,
   Author = {Thurman-Keup, RM and Kotwal, AV and Tecchio, M and Byon-Wagner,
             A},
   Title = {W boson physics at hadron colliders},
   Journal = {Reviews of Modern Physics},
   Volume = {73},
   Number = {2},
   Pages = {267-306},
   Publisher = {American Physical Society (APS)},
   Year = {2001},
   Month = {April},
   url = {http://dx.doi.org/10.1103/RevModPhys.73.267},
   Abstract = {The use of hadron colliders to investigate the properties of
             the W bosons started in 1982 at the CERN Spp̄S collider.
             Since then, the Tevatron experiments at Fermilab have
             recorded a large sample of W events which allowed precision
             measurements of the properties of W bosons. In this paper
             the authors review W gauge boson physics at hadron colliders
             from 1982 to 2000. They first discuss the production
             mechanism and detection of W bosons in pp̄ collisions.
             After a brief review of the early studies, W boson physics
             at the Tevatron collider are thoroughly examined. Finally,
             possible future directions of W boson physics at hadron
             colliders are discussed.},
   Doi = {10.1103/RevModPhys.73.267},
   Key = {fds308193}
}

@article{fds331625,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'Errico, M},
   Title = {W-boson polarization measurement in the tt- dilepton channel
             using the CDF II detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {722},
   Number = {1-3},
   Pages = {48-54},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.03.032},
   Abstract = {We present a measurement of the W-boson polarization in
             top-quark decays in tt- events with decays to dilepton final
             states using data corresponding to 5.1 fb-1 of integrated
             luminosity in pp- collisions collected by the CDF II
             detector at the Tevatron. Assuming a top-quark mass of 172.5
             GeV/c2, a simultaneous measurement of the fractions of
             longitudinal ( f0) and right-handed ( f+) W-bosons yields
             the results f0 = 0.70-0.17+0.18 (stat) ± 0.06(syst) and f+
             =-0.09 ± 0.09(stat) ± 0.03(syst). Combining this
             measurement with our previous measurement based on
             single-lepton final states, we obtain f0 = 0.84 ±
             0.09(stat) ± 0.05(syst) and f+ =-0.16 ± 0.05(stat) ±
             0.04(syst). The results are consistent with the standard
             model expectation.},
   Doi = {10.1016/j.physletb.2013.03.032},
   Key = {fds331625}
}

@article{fds356537,
   Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
             B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
             S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
             MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
             Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
             Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
             JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
             MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
             M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
             JP},
   Title = {Z boson production in Pb+Pb collisions at √Snn
             = 5.02 TeV measured by the ATLAS experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {802},
   Year = {2020},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2020.135262},
   Abstract = {The production yield of Z bosons is measured in the electron
             and muon decay channels in Pb+Pb collisions at √Snn = 5.02
             TeV with the ATLAS detector. Data from the 2015 LHC run
             corresponding to an integrated luminosity of 0.49 nb-1 are
             used for the analysis. The Z boson yield, normalised by the
             total number of minimum-bias events and the mean nuclear
             thickness function, is measured as a function of dilepton
             rapidity and event centrality. The measurements in Pb+Pb
             collisions are compared with similar measurements made in
             proton-proton collisions at the same centre-of-mass energy.
             The nuclear modification factor is found to be consistent
             with unity for all centrality intervals. The results are
             compared with theoretical predictions obtained at
             next-to-leading order using nucleon and nuclear parton
             distribution functions. The normalised Z boson yields in
             Pb+Pb collisions lie 1-3σ above the predictions. The
             nuclear modification factor measured as a function of
             rapidity agrees with unity and is consistent with a
             next-to-leading-order QCD calculation including the isospin
             effect.},
   Doi = {10.1016/j.physletb.2020.135262},
   Key = {fds356537}
}

@article{fds356705,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
             SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and AdamczyK, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and AfiK, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
             J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
             ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and AriK, M and Armbruster, AJ and Armitage, LJ},
   Title = {Z Z → + - ′ + ′ - s-section measurements and search
             for anomalous triple gauge couplings in 13 TeV p p
             collisions with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {97},
   Number = {3},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.97.032005},
   Abstract = {Measurements of ZZ production in the +-′+′- channel in
             proton-proton collisions at 13 TeV center-of-mass energy at
             the Large Hadron Collider are presented. The data correspond
             to 36.1 fb-1 of collisions collected by the ATLAS experiment
             in 2015 and 2016. Here and ′ stand for electrons or muons.
             Integrated and differential ZZ→+-′+′- cross sections
             with Z→+- candidate masses in the range of 66 GeV to 116
             GeV are measured in a fiducial phase space corresponding to
             the detector acceptance and corrected for detector effects.
             The differential cross sections are presented in bins of
             twenty observables, including several that describe the jet
             activity. The integrated cross section is also extrapolated
             to a total phase space and to all standard model decays of Z
             bosons with mass between 66 GeV and 116 GeV, resulting in a
             value of 17.3±0.9[±0.6(stat)±0.5(syst)±0.6(lumi)] pb.
             The measurements are found to be in good agreement with the
             standard model. A search for neutral triple gauge couplings
             is performed using the transverse momentum distribution of
             the leading Z boson candidate. No evidence for such
             couplings is found and exclusion limits are set on their
             parameters.},
   Doi = {10.1103/PhysRevD.97.032005},
   Key = {fds356705}
}

@booklet{Abbott98k,
   Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
             V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
             P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
             SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
             Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
             HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros, Y and Dudko,
             LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E},
   Title = {[Formula presented] production in [Formula presented]
             collisions at [Formula presented] and limits on anomalous
             [Formula presented] and [Formula presented]
             couplings},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {57},
   Number = {7},
   Pages = {R3817-R3821},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.57.R3817},
   Abstract = {We present a study of (Formula presented) production in
             (Formula presented) collisions at (Formula presented) from
             97 (Formula presented) of data collected in the (Formula
             presented) (μμγ) decay channel with the D0 detector at
             Fermilab. The event yield and kinematic characteristics are
             consistent with the standard model predictions. We obtain
             limits on anomalous (Formula presented) and (Formula
             presented) couplings for form factor scales (Formula
             presented) and (Formula presented) Combining this analysis
             with our previous results yields 95% C.L. limits (Formula
             presented) (Formula presented) (Formula presented) and
             (Formula presented) for a form factor scale (Formula
             presented). © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.57.R3817},
   Key = {Abbott98k}
}

@article{fds308021,
   Author = {al, TAE},
   Title = {``Direct measurement of the $W$ boson width in $p\overline
             p$ Collisions at $\sqrt{s} = 1.8$ TeV,''},
   Journal = {Physical Review Letters},
   Volume = {85},
   Number = {7},
   Pages = {3347},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/physrevlett.100.071801},
   Abstract = {A direct measurement of the total decay width of the W boson
             Gamma(W) is presented using 350 pb(-1) of data from pp[over
             ] collisions at square root s = 1.96 TeV collected with the
             CDF II detector at the Fermilab Tevatron. The width is
             determined by normalizing predicted signal and background
             distributions to 230 185 W candidates decaying to enu and
             micronu in the transverse-mass region 50<M(T)<90 GeV and
             then fitting the predicted shape to 6055 events in the
             high-M(T) region, 90<M(T)<200 GeV. The result is
             Gamma(W)=2032 +/- 45(stat)+/-57(syst) MeV, consistent with
             the standard model expectation.},
   Doi = {10.1103/physrevlett.100.071801},
   Key = {fds308021}
}

@article{fds307935,
   Author = {al, TAE},
   Title = {``Search for the supersymmetric partner of the top quark in
             \pbp collisions at $\sqrt{s} = 1.8$ TeV,''},
   Journal = {Physical Review},
   Volume = {D63},
   Number = {9},
   Pages = {091101},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/PhysRevD.63.091101},
   Abstract = {We report on a search for the supersymmetric partner of the
             top quark (top squark) produced in [Formula Presented]
             events using [Formula Presented] of [Formula Presented]
             collisions at [Formula Presented] recorded with the Collider
             Detector at Fermilab. In the case of a light top squark, the
             decay of the top quark into a top squark plus the lightest
             supersymmetric particle (LSP) could have a significant
             branching ratio. The observed events are consistent with
             standard model [Formula Presented] production and decay.
             Hence, we set limits on the branching ratio of the top quark
             decaying into a top squark plus LSP, excluding branching
             ratios above 45% for a LSP mass up to [Formula Presented] ©
             2001 The American Physical Society.},
   Doi = {10.1103/PhysRevD.63.091101},
   Key = {fds307935}
}

@article{fds308022,
   Author = {Aaltonen, and T, and others},
   Title = {{Cross Section Constrained Top Quark Mass Measurement from
             Dilepton Events at the Tevatron}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {6},
   Pages = {062005},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.062005},
   Abstract = {We report the first top-quark mass measurement that uses a
             cross-section constraint to improve the mass determination.
             This measurement is made with a dilepton $t\bar{t}$ event
             candidate sample collected with the Collider Detector II at
             Fermilab. From a data sample corresponding to an integrated
             luminosity of 1.2 fb-1, we measure a top-quark mass of
             170.7-3.9+4.2(stat)\pm 2.6(syst)\pm 2.4(theory) GeV/c2. The
             measurement without the cross-section constraint is
             169.7-4.9+5.2(stat)\pm 3.1(syst) GeV/c2.},
   Doi = {10.1103/physrevlett.100.062005},
   Key = {fds308022}
}

@article{fds308045,
   Author = {Aaltonen, and T, and others},
   Title = {{Cross section measurements of high-pT dilepton final-state
             processes using a global fitting method}},
   Journal = {Phys. Rev.},
   Volume = {D78},
   Number = {1},
   Pages = {012003},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.012003},
   Abstract = {We present a new method for studying high-pT dilepton events
             $(e^\pm e^{-/+}, \mu^\pm \mu^{-/+}, e^\pm\mu^{-/+})$ and
             simultaneously extracting the production cross sections of
             $p\bar{p}$-->$t\bar{t}$, $p\bar{p}$-->W+W-, and
             $p\bar{p}$-->Z0-->tau+tau- at a center-of-mass energy of
             $\sqrt{s}=1.96$ TeV. We perform a likelihood fit to the
             dilepton data in a parameter space defined by the missing
             transverse energy and the number of jets in the event. Our
             results, which use 360 pb-1 of data recorded with the CDF II
             detector at the Fermilab Tevatron Collider, are
             sigma($t\bar{t}$)=8.5-2.2+2.7 pb, sigma(W+W-)=16.3-4.4+5.2
             pb, and sigma(Z0-->tau+tau-)=291-46+50 pb.},
   Doi = {10.1103/PhysRevD.78.012003},
   Key = {fds308045}
}

@article{fds308017,
   Author = {Aaltonen, and T, and others},
   Title = {{Evidence for D0-D0bar mixing using the CDF II
             Detector}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {12},
   Pages = {121802},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.121802},
   Abstract = {We measure the time dependence of the ratio of decay rates
             for the rare decay D0-->K+pi- to the Cabibbo-favored decay
             D0-->K-pi+. A signal of 12.7×103 D0-->K+pi- decays was
             obtained using the Collider Detector at Fermilab II detector
             at the Fermilab Tevatron with an integrated luminosity of
             1.5 fb-1. We measure the D0-[overline D]0 mixing parameters
             (RD,y[prime],x[prime]2), and find that the data are
             inconsistent with the no-mixing hypothesis with a
             probability equivalent to 3.8 Gaussian standard
             deviations.},
   Doi = {10.1103/physrevlett.100.121802},
   Key = {fds308017}
}

@article{fds308014,
   Author = {Aaltonen, and T, and others},
   Title = {{First Flavor-Tagged Determination of Bounds on Mixing-
             Induced CP Violation in Bs -> J/psi phi Decays}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {16},
   Pages = {161802},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.161802},
   Abstract = {This Letter describes the first determination of bounds on
             the CP-violation parameter 2betas using Bs0 decays in which
             the flavor of the bottom meson at production is identified.
             The result is based on approximately 2000 Bs0-->J/psiphi
             decays reconstructed in a 1.35 fb-1 data sample collected
             with the CDF II detector using $p\bar{p}$ collisions
             produced at the Fermilab Tevatron. We report confidence
             regions in the two-dimensional space of 2betas and the
             decay-width difference DeltaGamma. Assuming the standard
             model predictions of 2betas and DeltaGamma, the probability
             of a deviation as large as the level of the observed data is
             15%, corresponding to 1.5 Gaussian standard
             deviations.},
   Doi = {10.1103/physrevlett.100.161802},
   Key = {fds308014}
}

@article{fds308024,
   Author = {Aaltonen, and T, and others},
   Title = {{First observation of the decay $B^0_s \to D^-_s D^+_s$ and
             measurement of its branching ratio}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {2},
   Pages = {021803},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.021803},
   Abstract = {We report the observation of the exclusive decay
             Bs0-->Ds-Ds+ at the 7.5 standard deviation level using 355
             pb-1 of data collected by the CDF II detector in $p\bar{p}$
             collisions at $\sqrt{s}=1.96$ TeV at the Fermilab Tevatron.
             We measure the relative branching ratio [script
             B](Bs0-->Ds-Ds+)/[script B](B0-->D-Ds+) =1.44-0.44+0.48.
             Using the world average value for [script B](B0-->D-Ds+), we
             find [script B](Bs0-->Ds-Ds+) =(9.4-4.2+4.4)×10-3. This
             provides a lower bound DeltaGammasCP/Gammas> =2[script
             B](Bs0-->Ds-Ds+)>1.2×10-2 at 95% C.L.},
   Doi = {10.1103/physrevlett.100.021803},
   Key = {fds308024}
}

@article{fds308005,
   Author = {Aaltonen, and T, and others},
   Title = {{Forward-Backward Asymmetry in Top Quark Production in
             $p\bar{p}$ Collisions at $sqrt{s}=1.96$ TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {101},
   Number = {20},
   Pages = {202001},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.202001},
   Abstract = {We present measurements of the forward-backward charge
             asymmetry in top pair production using 1.9 fb-1 of
             $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV recorded with
             the Collider Detector at Fermilab II. Correcting for
             acceptance and measurement dilutions we obtain parton-level
             asymmetries of AFB$p\bar{p}$=0.17\pm 0.08 in the $p\bar{p}$
             frame and AFB$t\bar{t}$=0.24+/-0.14 in the $t\bar{t}$ frame.
             The values are consistent with the standard model
             expectation and disfavor exotic production mechanisms with
             significant negative values.},
   Doi = {10.1103/physrevlett.101.202001},
   Key = {fds308005}
}

@article{fds308038,
   Author = {Aaltonen, and T, and others},
   Title = {{Limits on the Production of Narrow $t\bar{t}$ Resonances in
             $p\bar{p}$ Collisions at $\sqrt{s}=1.96$
             TeV}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {5},
   Pages = {051102},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.051102},
   Abstract = {We search for evidence of resonant top quark pair production
             in 955 pb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
             recorded with the CDF II detector at the Fermilab Tevatron.
             For fully reconstructed candidate $t\bar{t}$ events
             triggered on leptons with large transverse momentum and
             containing at least one identified b-quark jet, we compare
             the invariant mass spectrum of $t\bar{t}$ pairs to the
             expected superposition of standard model $t\bar{t}$,
             non-$t\bar{t}$ backgrounds, and a simple resonance model
             based on a sequential Z[prime] boson. We establish upper
             limits for sigma($p\bar{p}$-->Z[prime])·Br(Z[prime]-->$t\bar{t}$)
             in the Z[prime] mass interval from 450 GeV/c2 to 900 GeV/c2.
             A topcolor leptophobic Z[prime] is ruled out below 720
             GeV/c2, and the cross section of any narrow Z[prime]-like
             state decaying to $t\bar{t}$ is found to be less than 0.64
             pb at 95% C.L. for MZ[prime] above 700 GeV/c2.},
   Doi = {10.1103/PhysRevD.77.051102},
   Key = {fds308038}
}

@article{fds308043,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of $b$-jet Shapes in Inclusive Jet Production
             in $p \bar{p}$ Collisions at $\sqrt{s}$ =
             1.96-TeV}},
   Journal = {Phys. Rev.},
   Volume = {D78},
   Number = {7},
   Pages = {072005},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.072005},
   Abstract = {We present a measurement of the shapes of b-jets using 300
             pb-1 of data obtained with the upgraded Collider Detector at
             Fermilab (CDF II) in $p \bar{p}$ collisions at
             center-of-mass energy $\sqrt{s}=1.96$ TeV. This measurement
             covers a wide transverse momentum range, from 52 to 300
             GeV/c. Samples of heavy-flavor enhanced jets together with
             inclusive jets are used to extract the average shapes of
             b-jets. The b-jets are expected to be broader than inclusive
             jets. Moreover, b-jets containing a single b-quark are
             expected to be narrower than those containing a $b \bar{b}$
             pair from gluon splitting. The measured b-jet shapes are
             found to be significantly broader than expected from the
             pythia and herwig Monte Carlo simulations. This effect may
             arise from an underestimation of the fraction of b-jets
             originating from gluon splitting in these simulations. The
             jet shape distributions provided in this paper could be
             compared to any full Monte Carlo simulation and could be
             used to further constrain the various parameters.},
   Doi = {10.1103/PhysRevD.78.072005},
   Key = {fds308043}
}

@article{fds308026,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of correlated b-bbar production in ${p
             \bar{p}}$ collisions at s**(1/2) = 1960 GeV}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {7},
   Pages = {072004},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.072004},
   Abstract = {We present a measurement of the correlated b[overline b]
             production cross section. The data used in this analysis
             were taken with the upgraded CDF detector (CDF II) at the
             Fermilab Tevatron collider, and correspond to an integrated
             luminosity of 742 pb-1. We utilize muon pairs with invariant
             mass 5=3 GeV/c and |eta|=2 GeV/c and |y| mu,[overline b] -->
             mu=1549\pm 133 pb. We compare this result with theoretical
             predictions and previous measurements. We also report the
             measurement of sigmac --> mu,[overline c] --> mu, a
             by-product of the study of the background to b[overline b]
             production.},
   Doi = {10.1103/PhysRevD.77.072004},
   Key = {fds308026}
}

@article{fds308018,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of Inclusive Jet Cross Sections in $Z/\gamma^*
             (\to ee)+$ jets Production in $p\bar{p}$ Collisions at
             $\sqrt{s}=1.96$ TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {10},
   Pages = {102001},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.102001},
   Abstract = {Inclusive jet cross sections in Z/gamma* events, with
             Z/gamma* decaying into an electron-positron pair, are
             measured as a function of jet transverse momentum and jet
             multiplicity in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
             with the upgraded Collider Detector at Fermilab in run II,
             based on an integrated luminosity of 1.7 fb-1. The
             measurements cover the rapidity region |yjet|Tjet>30 GeV/c.
             Next-to-leading order perturbative QCD predictions are in
             good agreement with the measured cross sections.},
   Doi = {10.1103/physrevlett.100.102001},
   Key = {fds308018}
}

@article{fds308016,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of Lifetime and Decay-Width Difference in
             $B^0_s \to J/\psi \phi$ Decays}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {12},
   Pages = {121803},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.121803},
   Abstract = {We measure the mean lifetime ${\tau=2/(\Gamma_L+\Gamma_H)}$
             and the decay-width difference ${\Delta\Gamma=\Gamma_L-\Gamma_H}$
             of the light and heavy mass eigenstates of the ${B_s^0}$
             meson, ${B_{sL}^0}$ and ${B_{sH}^0}$, in ${B_s^0\to
             J/\psi\phi}$ decays using 1.7 fb-1 of data collected with
             the CDF II detector at the Fermilab Tevatron $p\bar{p}$
             collider. Assuming CP conservation, a good approximation for
             the ${B_s^0}$ system in the standard model, we obtain
             ${\Delta\Gamma=0.076_{-0.063}^{+0.059}}$(stat)$\pm
             0.006$(syst) ps-1 and $\tau=1.52\pm 0.04$(stat)$\pm
             0.02$(syst) ps, the most precise measurements to date. Our
             constraints on the weak phase and ${\Delta\Gamma}$ are
             consistent with CP conservation.},
   Doi = {10.1103/physrevlett.100.121803},
   Key = {fds308016}
}

@article{fds308032,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of Ratios of Fragmentation Fractions for Bottom
             Hadrons in $p \bar{p}$ Collisions at $\sqrt{s}$ =
             1.96-TeV}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {7},
   Pages = {072003},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.072003},
   Abstract = {This paper describes the first measurement of b-quark
             fragmentation fractions into bottom hadrons in Run II of the
             Tevatron Collider at Fermilab. The result is based on a 360
             pb-1 sample of data collected with the CDF II detector in
             $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV. Semileptonic
             decays of [overline B]0, B-, and [overline B]s0 mesons, as
             well as Lambdab0 baryons, are reconstructed. For an
             effective bottom hadron pT threshold of 7 GeV/c, the
             fragmentation fractions are measured to be fu/fd=1.054\pm
             0.018(stat)-0.045+0.025(sys)\pm 0.058([script B]),
             fs/(fu+fd)=0.160\pm 0.005(stat)-0.010+0.011(sys)-0.034+0.057([script
             B]), and fLambdab/(fu+fd)=0.281\pm 0.012(stat)-0.056+0.058(sys)-0.087+0.128([script
             B]), where the uncertainty [script B] is due to
             uncertainties on measured branching ratios. The value of
             fs/(fu+fd) agrees within one standard deviation with
             previous CDF measurements and the world average of this
             quantity, which is dominated by LEP measurements. However,
             the ratio fLambdab/(fu+fd) is approximately twice the value
             previously measured at LEP. The approximately 2sigma
             discrepancy is examined in terms of kinematic differences
             between the two production environments.},
   Doi = {10.1103/PhysRevD.77.072003},
   Key = {fds308032}
}

@article{fds308041,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of the cross section for ${W}$-boson production
             in association with jets in $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {6},
   Pages = {011108},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1007/JHEP06(2013)084},
   Abstract = {We present a measurement of the cross section for W-boson
             production in association with jets in $p\bar{p}$ collisions
             at $\sqrt{s}=1.96$ TeV. The analysis uses a data sample
             corresponding to an integrated luminosity of 320 pb-1
             collected with the CDF II detector. W bosons are identified
             in their electron decay channel and jets are reconstructed
             using a cone algorithm. For each W+>=n-jet sample (n=1-4) we
             measure the differential cross section dsigma($p\bar{p}$-->W+>=n-jet)/dETnth-jet×[script
             B](W-->enu) with respect to the transverse energy ET of the
             nth-highest ET jet above 20 GeV, and the total cross section
             sigma($p\bar{p}$-->W+>=n-jet;ETnth-jet>25 GeV)×[script
             B](W-->enu), for a restricted W-->enu decay phase space. The
             cross sections, corrected for all detector effects, can be
             directly compared to particle level W+jet(s) predictions. We
             present here comparisons to leading order and
             next-to-leading order predictions.},
   Doi = {10.1007/JHEP06(2013)084},
   Key = {fds308041}
}

@article{fds308044,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of the Inclusive Jet Cross Section at the
             Fermilab Tevatron $p \bar{p}$ Collider Using a Cone-Based
             Jet Algorithm}},
   Journal = {Phys. Rev.},
   Volume = {D78},
   Number = {5},
   Pages = {052006},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.052006},
   Abstract = {We present a measurement of the inclusive jet cross section
             in $p \bar{p}$ collisions at $\sqrt{s}=1.96$ TeV based on
             data collected by the CDF II detector with an integrated
             luminosity of 1.13 fb-1. The measurement was made using the
             cone-based midpoint jet clustering algorithm in the rapidity
             region of |y|},
   Doi = {10.1103/PhysRevD.78.052006},
   Key = {fds308044}
}

@article{fds308029,
   Author = {Aaltonen, and T, and others},
   Title = {{Model-Independent and Quasi-Model-Independent Search for
             New Physics at CDF}},
   Journal = {Phys. Rev.},
   Volume = {D78},
   Number = {1},
   Pages = {012002},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.012002},
   Abstract = {Data collected in run II of the Fermilab Tevatron are
             searched for indications of new electroweak scale physics.
             Rather than focusing on particular new physics scenarios,
             CDF data are analyzed for discrepancies with respect to the
             standard model prediction. A model-independent approach
             (Vista) considers the gross features of the data and is
             sensitive to new large cross section physics. A
             quasi-model-independent approach (Sleuth) searches for a
             significant excess of events with large summed transverse
             momentum and is particularly sensitive to new electroweak
             scale physics that appears predominantly in one final state.
             This global search for new physics in over 300 exclusive
             final states in 927 pb-1 of $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV reveals no such significant indication
             of physics beyond the standard model.},
   Doi = {10.1103/PhysRevD.78.012002},
   Key = {fds308029}
}

@article{fds308034,
   Author = {Aaltonen, and T, and others},
   Title = {{Observation of Exclusive Dijet Production at the Fermilab
             Tevatron ${p \bar{p}}$ Collider}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {5},
   Pages = {052004},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.052004},
   Abstract = {We present the first observation and cross section
             measurement of exclusive dijet production in [overline p]p
             interactions, [overline p]p-->[overline p]+dijet+p. Using a
             data sample of 310 pb-1 collected by the Run II Collider
             Detector at Fermilab at $\sqrt{s}=1.96$ TeV, exclusive cross
             sections for events with two jets of transverse energy
             ETjet>=10 GeV have been measured as a function of minimum
             ETjet. The exclusive signal is extracted from fits to data
             distributions based on Monte Carlo simulations of expected
             dijet signal and background shapes. The simulated background
             distribution shapes are checked in a study of a largely
             independent data sample of 200 pb-1 of b-tagged jet events,
             where exclusive dijet production is expected to be
             suppressed by the Jz=0 total angular momentum selection
             rule. Results obtained are compared with theoretical
             expectations, and implications for exclusive Higgs boson
             production at the pp Large Hadron Collider at sqrt(s)=14 TeV
             are discussed.},
   Doi = {10.1103/PhysRevD.77.052004},
   Key = {fds308034}
}

@article{fds308020,
   Author = {Aaltonen, and T, and others},
   Title = {{Observation of Orbitally Excited ${B_s}$
             Mesons}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {8},
   Pages = {082001},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.082001},
   Abstract = {We report the observation of two narrow resonances
             consistent with states of orbitally excited (L=1) Bs mesons
             using 1 fb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
             collected with the Collider Detector at Fermilab II detector
             at the Fermilab Tevatron. We use two-body decays into K- and
             B+ mesons reconstructed as B+-->J/psiK+, J/psi-->\mu^+\mu^-
             or B+-->[overline D]0pi+, [overline D]0-->K+pi-. We deduce
             the masses of the two states to be m(Bs1)=5829.4\pm 0.7
             MeV/c2 and m(Bs2*)=5839.6\pm 0.7 MeV/c2.},
   Doi = {10.1103/physrevlett.100.082001},
   Key = {fds308020}
}

@article{fds308031,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for chargino-neutralino production in ${p \bar{p}}$
             collisions at 1.96 TeV with high pT leptons}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {5},
   Pages = {052002},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.052002},
   Abstract = {We present a search for the associated production of
             charginos and neutralinos in $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV. The data were collected at the Collider
             Detector at Fermilab (CDF II) and correspond to integrated
             luminosities between 0.7 and 1.0 fb-1. We look for final
             states with one high-pT electron or muon, and two additional
             leptons. Our results are consistent with the standard model
             expectations, and we set limits on the cross section as a
             function of the chargino mass in three different
             supersymmetric scenarios. For a specific minimal
             supersymmetric standard model scenario with no slepton
             mixing, we set a 95% C.L. limit at 151 GeV/c2.},
   Doi = {10.1103/PhysRevD.77.052002},
   Key = {fds308031}
}

@article{fds308009,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for Doubly Charged Higgs Bosons with Lepton-Flavor-
             Violating Decays involving Tau Leptons}},
   Journal = {Phys. Rev. Lett.},
   Volume = {101},
   Number = {12},
   Pages = {121801},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.121801},
   Abstract = {We search for pair production of doubly charged Higgs
             particles ($H^{\pm\pm}$) followed by decays into
             electron-tau (etau) and muon-tau (mu tau) pairs using data
             (350 pb-1) collected from $\bar{p} p$ collisions at
             $\sqrt{s}=1.96$ TeV by the CDF II experiment. We search
             separately for cases where three or four final-state leptons
             are detected, and combine results for exclusive decays to
             left-handed etau (\mu tau) pairs. We set an $H^{\pm\pm}$
             lower mass limit of 114(112) GeV/c2 at the 95% confidence
             level.},
   Doi = {10.1103/physrevlett.101.121801},
   Key = {fds308009}
}

@article{fds308015,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for Heavy Top-like Quarks Using Lepton Plus Jets
             Events in 1.96-TeV $p \bar{p}$ Collisions}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {16},
   Pages = {161803},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.161803},
   Abstract = {We present the results of a search for pair production of a
             new heavy toplike quark t[prime] decaying to a ${W}$ boson
             and another quark using the Collider Detector at Fermilab II
             detector in run II of the Tevatron $p\bar{p}$ collider.
             Using a data sample corresponding to 760 pb-1 of integrated
             luminosity, we fit the observed spectrum of total transverse
             energy and reconstructed t[prime] quark mass to a
             combination of standard model processes and t[prime] pair
             production. We see no evidence for t[prime][overline
             t][prime] production, and we infer a lower limit of 256
             GeV/c2 on the mass of the t[prime] at 95% C.L. assuming
             standard strong couplings for the t[prime].},
   Doi = {10.1103/physrevlett.100.161803},
   Key = {fds308015}
}

@article{fds308042,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for Heavy, Long-Lived Neutralinos that Decay to
             Photons at CDF II Using Photon Timing}},
   Journal = {Phys. Rev.},
   Volume = {D78},
   Number = {3},
   Pages = {032015},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.032015},
   Abstract = {We present the results of the first hadron collider search
             for heavy, long-lived neutralinos that decay via
             chi-tilde10-->gammaG-tilde in gauge-mediated supersymmetry
             breaking models. Using an integrated luminosity of 570\pm 34
             pb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV, we
             select gamma+jet+missing transverse energy candidate events
             based on the arrival time of a high-energy photon at the
             electromagnetic calorimeter as measured with a timing system
             that was recently installed on the CDF II detector. We find
             2 events, consistent with the background estimate of 1.3\pm
             0.7 events. While our search strategy does not rely on
             model-specific dynamics, we set cross section limits and
             place the world-best 95% C.L. lower limit on the chi-tilde10
             mass of 101 GeV/c2 at tauchi-tilde[sub 1][sup 0]=5
             ns.},
   Doi = {10.1103/PhysRevD.78.032015},
   Key = {fds308042}
}

@article{fds308008,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for large extra dimensions in final states
             containing one photon or jet and large missing transverse
             energy produced in $p \bar{p}$ collisions at $\sqrt{s}$ =
             1.96-TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {101},
   Number = {18},
   Pages = {181602},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.181602},
   Abstract = {We present the results of searches for large extra
             dimensions in samples of events with large missing
             transverse energy E-slash T and either a photon or a jet
             produced in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
             collected with the Collider Detector at Fermilab II. For
             gamma+E-slash T and jet+E-slash T candidate samples
             corresponding to 2.0 and 1.1 fb-1 of integrated luminosity,
             respectively, we observe good agreement with standard model
             expectations and obtain a combined lower limit on the
             fundamental parameter of the large extra dimensions model MD
             as a function of the number of extra dimensions in the
             model.},
   Doi = {10.1103/physrevlett.101.181602},
   Key = {fds308008}
}

@article{fds308033,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for New Heavy Particles Decaying to $Z^0 Z^0 \to
             eeee$ in $p$ - $\bar{p}$ Collisions at $\sqrt{s}$ = 1.96-
             TeV}},
   Journal = {Phys. Rev.},
   Volume = {D78},
   Number = {1},
   Pages = {012008},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.012008},
   Abstract = {We report the results of a search for the anomalous
             production of a massive particle decaying to four electrons
             via two Z0 bosons in 1.1 fb-1 of $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV collected by the CDF II detector at
             Fermilab. We employ optimized electron identification
             criteria to maximize acceptance and efficiency. We estimate
             the backgrounds in the invariant mass range 500–1000
             GeV/c2 to be 0.028\pm 0.009(stat)\pm 0.011(syst) events. We
             observe zero events in this search region. Assuming a
             Randall-Sundrum graviton production model, we set 95% C.L.
             limits on sigma×BF(G-->Z0Z0)},
   Doi = {10.1103/PhysRevD.78.012008},
   Key = {fds308033}
}

@article{fds308010,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for Pair Production of Scalar Top Quarks Decaying to
             a $\tau$ Lepton and a $b$ Quark in $p\bar{p}$ Collisions at
             sqrt{s}=1.96 TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {101},
   Number = {7},
   Pages = {071802},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.071802},
   Abstract = {We search for pair production of supersymmetric top quarks
             (t-tilde1), followed by R-parity violating decay
             t-tilde1-->taub with a branching ratio beta, using 322 pb-1
             of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV collected by
             the upgraded Collider Detector at Fermilab. Two candidate
             events pass our final selection criteria, consistent with
             the standard model expectation. We set upper limits on the
             cross section sigma(t-tilde1[overline t-tilde ]1)×beta2 as
             a function of the top-squark mass m(t-tilde1). Assuming
             beta=1, we set a 95% confidence level limit m(t-tilde1)>153
             GeV/c2. The limits are also applicable to the case of a
             third-generation scalar leptoquark (LQ3) decaying
             LQ3-->taub.},
   Doi = {10.1103/physrevlett.101.071802},
   Key = {fds308010}
}

@article{fds308028,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for resonant $t \bar{t}$ production in $p \bar{p}$
             collisions at $\sqrt{s}$ = 1.96-TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {23},
   Pages = {231801},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.231801},
   Abstract = {We report on a search for narrow-width particles decaying to
             a top and antitop quark pair. The data set used in the
             analysis corresponds to an integrated luminosity of 680 pb-1
             collected with the Collider Detector at Fermilab in run II.
             We present 95% confidence level upper limits on the cross
             section times branching ratio. Assuming a specific
             top-color-assisted technicolor production model, the
             leptophobic Z[prime] with width GammaZ[prime]=0.012MZ[prime],
             we exclude the mass range MZ[prime]},
   Doi = {10.1103/physrevlett.100.231801},
   Key = {fds308028}
}

@article{fds308023,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for Standard Model Higgs Bosons Produced in
             Association with ${W}$ Bosons}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {4},
   Pages = {041801},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.041801},
   Abstract = {We report the observation of two narrow resonances
             consistent with states of orbitally excited (L=1) Bs mesons
             using 1 fb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
             collected with the Collider Detector at Fermilab II detector
             at the Fermilab Tevatron. We use two-body decays into K- and
             B+ mesons reconstructed as B+-->J/psiK+, J/psi-->\mu +\mu -
             or B+-->[overline D]0pi+, [overline D]0-->K+pi-. We deduce
             the masses of the two states to be m(Bs1)=5829.4\pm 0.7
             MeV/c2 and m(Bs2*)=5839.6\pm 0.7 MeV/c2.},
   Doi = {10.1103/physrevlett.100.041801},
   Key = {fds308023}
}

@article{fds308012,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for the Higgs boson in events with missing
             transverse energy and $b$ quark jets produced in proton-
             antiproton collisions at $\sqrt{s}$ =1.96
             TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {21},
   Pages = {211801},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.211801},
   Abstract = {We search for the standard model Higgs boson produced in
             association with an electroweak vector boson in events with
             no identified charged leptons, large imbalance in transverse
             momentum, and two jets where at least one contains a
             secondary vertex consistent with the decay of b hadrons. We
             use ~1 fb-1 integrated luminosity of $p\bar{p}$ collisions
             at $\sqrt{s}=1.96$ TeV recorded by the Collider Detector at
             Fermilab II experiment at the Tevatron. We find 268 (16)
             single (double) b-tagged candidate events, where $248\pm 43$
             ($14.4\pm 2.7$) are expected from standard model background
             processes. We observe no significant excess over the
             expected background and thus set 95% confidence level upper
             limits on the Higgs boson production cross section for
             several Higgs boson masses ranging from 110 to 140 GeV/c2.
             For a mass of 115 GeV/c2, the observed (expected) limit is
             20.4 (14.2) times the standard model prediction.},
   Doi = {10.1103/physrevlett.100.211801},
   Key = {fds308012}
}

@article{fds308025,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for third generation vector leptoquarks in
             $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.96-TeV}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {9},
   Pages = {091105},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.091105},
   Abstract = {We search for a third generation vector leptoquark (VLQ3)
             that decays to a $b$ quark and tau lepton using the CDF II
             detector and 320 pb-1 of integrated luminosity from the
             Fermilab Tevatron. Observing a number of events in agreement
             with standard model expectations, we obtain, assuming
             Yang-Mills (minimal) couplings, the most stringent upper
             limit on the VLQ3 pair production cross section of 344 fb
             (493 fb) and lower limit on the VLQ3 mass of 317 GeV/c2 (251
             GeV/c2) at 95% C.L.},
   Doi = {10.1103/PhysRevD.77.091105},
   Key = {fds308025}
}

@article{fds308013,
   Author = {Aaltonen, and T, and others},
   Title = {{Strong Evidence for $Z Z$ Production in panti-p Collisions
             at $\sqrt{s}$ = 1.96-TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {20},
   Pages = {201801},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.201801},
   Abstract = {We report the first evidence of Z boson pair production at a
             hadron collider with a significance exceeding 4 standard
             deviations. This result is based on a data sample
             corresponding to 1.9 fb-1 of integrated luminosity from
             $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV collected with
             the Collider Detector at Fermilab II detector. In the
             [script-l][script-l][script-l][prime][script-l][prime]
             channel, we observe three ZZ candidates with an expected
             background of 0.096-0.063+0.092 events. In the
             [script-l][script-l]nunu channel, we use a leading-order
             calculation of the relative ZZ and WW event probabilities to
             discriminate between signal and background. In the
             combination of [script-l][script-l][script-l][prime][script-l][prime]
             and [script-l][script-l]nunu channels, we observe an excess
             of events with a probability of 5.1×10-6 to be due to the
             expected background. This corresponds to a significance of
             4.4 standard deviations. The measured cross section is
             sigma($p\bar{p}$-->ZZ)=1.4-0.6+0.7(stat+syst) pb, consistent
             with the standard model expectation.},
   Doi = {10.1103/physrevlett.100.201801},
   Key = {fds308013}
}

@article{fds308037,
   Author = {Aaltonen, and T, and others},
   Title = {{Two-particle momentum correlations in jets produced in $p
             \bar{p}$ Collisions at $\sqrt{s}$ = 1.96-TeV}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {9},
   Pages = {092001},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.092001},
   Abstract = {We present the first measurement of two-particle momentum
             correlations in jets produced in $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV. Results are obtained for charged
             particles within a restricted cone with an opening angle of
             0.5 radians around the jet axis and for events with dijet
             masses between 66 and 563 GeV/c2. A comparison of the
             experimental data to theoretical predictions obtained for
             partons within the framework of resummed perturbative QCD in
             the next-to-leading log approximation shows that the parton
             momentum correlations survive the hadronization stage of jet
             fragmentation, giving further support to the hypothesis of
             local parton-hadron duality. The extracted value of the
             next-to-leading-log-approximation parton shower cutoff scale
             Qeff set equal to LambdaQCD is found to be
             (1.4-0.7+0.9)×100 MeV.},
   Doi = {10.1103/PhysRevD.77.092001},
   Key = {fds308037}
}

@article{fds308210,
   Author = {Adams, MR and Aderholz, M and Aïd, S and Anthony, PL and Ashery, D and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dietrich, FS and Dougherty, W and Dreyer,
             T and Eckardt, V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen, KA and Guo,
             RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Jackson,
             HE and Jancso, G and Jansen, DM and Jin, Z and Kadija, K and Kaufmann, S and Kennedy, RD and Kinney, ER and Kobrak, HGE and Kotwal, AV and Kunori, S and Lenski, M and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin,
             JG and Nickerson, RB and Novak, J and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou, V and Pawlik, B and Pipkin, FM and Potterveld, DH and Röser, A and Ryan, JJ and Salgado, CW and Schellman,
             H and Schmitt, M and Schmitz, N and Siegert, G and Skuja, A and Snow, GA and Söldner-Rembold, S and Spentzouris, P and Stopa, P and Swanson, RA and Topor Pop and V and Venkataramania, H and Wilhelm, M and Wilson, R and Wittek, W and Wolbers, SA and Zghiche, A and Zhao,
             T},
   Title = {Λ and Λ̄ polarization from deep inelastic muon
             scattering},
   Journal = {European Physical Journal C},
   Volume = {17},
   Number = {2},
   Pages = {263-267},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1007/s100520000493},
   Abstract = {We report results of the first measurements of Λ and Λ̄
             polarization produced in deep inelastic polarized muon
             scattering on the nucleon. The results are consistent with
             an expected trend towards positive polarization with
             increasing cursive Greek chiF. The polarizations of Λ and
             Λ̄ appear to have opposite signs. A large negative
             polarization for Λ at low positive cursive Greek chiF is
             observed and is not explained by existing models. A possible
             interpretation is presented.},
   Doi = {10.1007/s100520000493},
   Key = {fds308210}
}


%% Papers Accepted   
@article{fds375049,
   Author = {A.V. Kotwal and the ATLAS Collaboration},
   Title = {Search for top-philic heavy resonances in pp collisions at
             √s = 13 TeV with the ATLAS detector},
   Publisher = {European Physics Journal C},
   Year = {2023},
   Month = {Winter},
   url = {https://doi.org/10.48550/arXiv.2304.01678},
   Key = {fds375049}
}


%% Papers Submitted   
@article{fds354061,
   Author = {G. Aad et al (ATLAS Collaboration)},
   Title = {Jet energy scale and resolution measured in proton-proton
             collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {European Physics Journal C},
   Year = {2020},
   Month = {July},
   Key = {fds354061}
}

@article{fds354062,
   Author = {G. Aad et al (ATLAS Collaboration)},
   Title = {Search for displaced leptons in √s=13 TeV pp collisions
             with the ATLAS detector},
   Journal = {Physical Review Letters},
   Year = {2020},
   Month = {November},
   Key = {fds354062}
}


%% Preprints   
@article{fds347562,
   Author = {A.V. Kotwal},
   Title = {A fast method for finding charged-particle trajectories
             using unsupervised machine learning embedded in
             field-programmable gate arrays},
   Year = {2019},
   Month = {October},
   url = {http://arxiv.org/abs/1910.14149v1},
   Key = {fds347562}
}

@article{fds221253,
   Author = {A.V. Kotwal and the ATLAS Collaboration},
   Title = {Beyond Standard Model Higgs boson searches at a
             High-Luminosity LHC with ATLAS},
   Journal = {ATL-PHYS-PUB-2013-016},
   Year = {2013},
   Month = {October},
   Key = {fds221253}
}

@article{fds221248,
   Author = {A.V. Kotwal and the ATLAS Collaboration},
   Title = {Studies of Sensitivity to New Dilepton and Ditop Resonances
             with an Upgraded ATLAS Detector at a High-Luminosity
             LHC},
   Journal = {ATLAS-PHYS-PUB-2013-003},
   Year = {2013},
   Month = {February},
   Key = {fds221248}
}

@article{fds221250,
   Author = {A.V. Kotwal and the ATLAS Collaboration},
   Title = {Studies of Vector Boson Scattering And Triboson Production
             with an Upgraded ATLAS Detector at a High-Luminosity
             LHC},
   Journal = {ATL-PHYS-PUB-2013-006},
   Year = {2013},
   Month = {June},
   Key = {fds221250}
}

@article{fds221249,
   Author = {A.V. Kotwal and C. Degrange et al.},
   Title = {Studies of Vector Boson Scattering And Triboson Production
             with DELPHES Parametrized Fast Simulation for Snowmass
             2013},
   Journal = {arXiv:1309.7452},
   Year = {2013},
   Month = {October},
   Key = {fds221249}
}